Bulk acoustic wave resonator filters including rejection-band resonators

ABSTRACT

A Bulk Acoustic Wave (BAW) resonator filter can include a BAW resonator pass-band filter ladder, where the BAW resonator pass-band filter ladder can be configured to pass frequency components of an input signal in a pass-band of frequencies received at an input node of the BAW resonator pass-band filter ladder to an output node of the BAW resonator pass-band filter ladder. A first rejection-band series resonator can be coupled in series between an input port of the BAW resonator pass-band filter ladder and the input node, where the first rejection-band series resonator can have a first anti-resonant frequency peak in a rejection-band of frequencies that is less than the pass-band of frequencies. A second rejection-band series resonator can be coupled in series between an output port of the BAW resonator filter and the output node, where the second rejection-band series resonator can have a second anti-resonant frequency peak in the rejection-band of frequencies.

CROSS-REFERENCES TO RELATED APPLICATIONS

The present application claims priority to U.S Provisional Application Ser. No. 62/845,009 entitled “WiFi 5 GHz NEW APPROACH FOR REJECTION IMPROVEMENT,” filed in the U.S.P.T.O. on May 8, 2019 and to U.S Provisional Application Ser. No. 62/885,047 entitled “BULK ACOUSTIC WAVE RESONATOR FILTERS INCLUDING REJECTION-BAND RESONATORS,” filed in the U.S.P.T.O. on Aug. 9, 2019, and is a continuation-in-part application of U.S. patent application Ser. No. 16/135,276, titled “FRONT END MODULE FOR 5.2 GHZ WI-FI ACOUSTIC WAVE RESONATOR RF FILTER CIRCUIT,” filed Sep. 19, 2018, which is a continuation-in-part application of U.S. patent application Ser. No. 16/019,267, titled “5.2 GHz Wi-Fi ACOUSTIC WAVE RESONATOR RF FILTER CIRCUIT,” filed Jun. 26, 2018, which is a continuation-in-part application of U.S. patent application Ser. No. 15/784,919, titled “PIEZOELECTRIC ACOUSTIC RESONATOR MANUFACTURED WITH PIEZOELECTRIC THIN FILM TRANSFER PROCESS,” filed Oct. 16, 2017, which is a continuation-in-part of U.S. application Ser. No. 15/068,510 filed Mar. 11, 2016.

The present application incorporates by reference, for all purposes, the following concurrently filed patent applications, all commonly owned: U.S. patent application Ser. No. 14/298,057, titled “RESONANCE CIRCUIT WITH A SINGLE CRYSTAL CAPACITOR DIELECTRIC MATERIAL”, filed Jun. 6, 2014 (now U.S. Pat. No. 9,673,384 issued Jun. 6, 2017); U.S. patent application Ser. No. 14/298,076, titled “METHOD OF MANUFACTURE FOR SINGLE CRYSTAL CAPACITOR DIELECTRIC FOR A RESONANCE CIRCUIT”, filed Jun. 6, 2014 (now U.S. Pat. No. 9,537,465 issued Jan. 3, 2017); U.S. patent application Ser. No. 14/298,100, titled “INTEGRATED CIRCUIT CONFIGURED WITH TWO OR MORE SINGLE CRYSTAL ACOUSTIC RESONATOR DEVICES”, filed Jun. 6, 2014 (now U.S. Pat. No. 9,571,061 issued Feb. 14, 2017); U.S. patent application Ser. No. 14/341,314, titled “WAFER SCALE PACKAGING”, filed Jul. 25, 2014 (now U.S. Pat. No. 9,805,966 issued Oct. 31, 2017); U.S. patent application Ser. No. 14/449,001, titled “MOBILE COMMUNICATION DEVICE CONFIGURED WITH A SINGLE CRYSTAL PIEZO RESONATOR STRUCTURE”, filed Jul. 31, 2014 (now U.S. Pat. No. 9,716,581 issued Jul. 25, 2017); U.S. patent application Ser. No. 14/469,503, titled “MEMBRANE SUBSTRATE STRUCTURE FOR SINGLE CRYSTAL ACOUSTIC RESONATOR DEVICE”, filed Aug. 26, 2014 (now U.S. Pat. No. 9,917,568 issued Mar. 13, 2018). The disclosures of all of the above applications and patents are incorporated herein by reference.

BACKGROUND

The present invention relates generally to electronic devices. More particularly, the present invention provides techniques related to a method of manufacture and a structure for bulk acoustic wave resonator devices, single crystal bulk acoustic wave resonator devices, single crystal filter and resonator devices, and the like. Merely by way of example, the invention has been applied to a single crystal resonator device for a communication device, mobile device, computing device, among others.

Mobile telecommunication devices have been successfully deployed world-wide. Over a billion mobile devices, including cell phones and smartphones, were manufactured in a single year and unit volume continues to increase year-over-year. With ramp of 4G/LTE in about 2012, and explosion of mobile data traffic, data rich content is driving the growth of the smartphone segment—which is expected to reach 2B per annum within the next few years. Coexistence of new and legacy standards and thirst for higher data rate requirements is driving RF complexity in smartphones. Unfortunately, limitations exist with conventional RF technology that is problematic, and may lead to drawbacks in the future.

With 4G LTE and 5G growing more popular by the day, wireless data communication demands high performance RF filters with frequencies around 5 GHz and higher. Bulk acoustic wave resonators (BAWR) using crystalline piezoelectric thin films are leading candidates for meeting such demands. Current BAWRs using polycrystalline piezoelectric thin films are adequate for bulk acoustic wave (BAW) filters operating at frequencies ranging from 1 to 3 GHz; however, the quality of the polycrystalline piezoelectric films degrades quickly as the thicknesses decrease below around 0.5 um, which is required for resonators and filters operating at frequencies around 5 GHz and above. Single crystalline or epitaxial piezoelectric thin films grown on compatible crystalline substrates exhibit good crystalline quality and high piezoelectric performance even down to very thin thicknesses, e.g., 0.4 um. Even so, there are challenges to using and transferring single crystal piezoelectric thin films in the manufacture of BAWR and BAW filters.

SUMMARY

Embodiments according to the invention can provide bulk acoustic wave resonator filters including rejection-band resonators. Pursuant to these embodiments, in some embodiments according to the invention, a Bulk Acoustic Wave (BAW) resonator filter can include a BAW resonator pass-band filter circuit, the BAW resonator pass-band filter circuit configured to pass frequency components of an input signal in a pass-band of frequencies received at an input node of the BAW resonator pass-band filter circuit to an output node of the BAW resonator pass-band filter circuit. A first rejection-band series resonator can be coupled in series between an input port of the BAW resonator pass-band filter circuit and the input node, the first rejection-band series resonator having a first anti-resonant frequency peak in a rejection-band of frequencies that is less than the pass-band of frequencies. A second rejection-band series resonator can be coupled in series between an output port of the BAW resonator filter and the output node, the second rejection-band series resonator having a second anti-resonant frequency peak in the rejection-band of frequencies.

In some embodiments according to the invention, a Bulk Acoustic Wave (BAW) resonator filter can include a BAW resonator pass-band filter circuit, the BAW resonator pass-band filter circuit configured to pass frequency components of an input signal in a pass-band of frequencies received at an input port of the BAW resonator pass-band filter circuit to an output port of the BAW resonator pass-band filter circuit. A first rejection-band shunt resonator can be coupled in parallel across an input port of the BAW resonator pass-band filter circuit and a reference node of the BAW resonator pass-band filter circuit, the first rejection-band shunt resonator having a first resonant frequency peak in a rejection-band of frequencies that is greater than the pass-band of frequencies. A second rejection-band shunt resonator can be coupled in parallel between the output port of the BAW resonator filter and the reference node, the second rejection-band shunt resonator having a second resonant frequency peak in the rejection-band of frequencies.

In some embodiments according to the invention, a Bulk Acoustic Wave (BAW) resonator filter can include a BAW resonator pass-band filter circuit, the BAW resonator pass-band filter circuit configured to pass frequency components of an input signal in a pass-band of frequencies received at an input node of the BAW resonator pass-band filter circuit to an output node of the BAW resonator pass-band filter circuit. A first rejection-band series resonator can be coupled in series with an input port of the BAW resonator pass-band filter circuit or an output port of the BAW resonator pass-band filter circuit, the first rejection-band series resonator having a first anti-resonant frequency peak in a rejection-band of frequencies that is less than the pass-band of frequencies.

In some embodiments according to the invention, a Bulk Acoustic Wave (BAW) resonator filter can include a BAW resonator pass-band filter circuit configured to pass frequency components of an input signal in a pass-band of frequencies received at an input port of the BAW resonator pass-band filter circuit to an output port of the BAW resonator pass-band filter circuit. A first rejection-band shunt resonator can be coupled in parallel across an input port of the BAW resonator pass-band filter circuit and a reference node of the BAW resonator pass-band filter circuit or coupled in parallel between the output port of the BAW resonator filter and the reference node, the first rejection-band shunt resonator having a first resonant frequency peak in a rejection-band of frequencies that is greater than the pass-band of frequencies.

In some embodiments according to the invention, a Bulk Acoustic Wave (BAW) resonator filter can include a first BAW resonator pass-band filter circuit configured to pass frequency components of an input signal in a first pass-band of frequencies received at an input port of the first BAW resonator pass-band filter circuit to an output port of the first BAW resonator pass-band filter circuit. A first rejection-band series resonator can be coupled in series with the input port of the BAW resonator pass-band filter circuit or the output port of the BAW resonator pass-band filter circuit, the first rejection-band series resonator having a first anti-resonant frequency peak in a first rejection-band of frequencies that is less than the first pass-band of frequencies. A second BAW resonator pass-band filter circuit can be configured to pass frequency components of the input signal in a second pass-band of frequencies received at the input port of the second BAW resonator pass-band filter circuit to the output port of the second BAW resonator pass-band filter circuit. A first rejection-band shunt resonator cane be coupled in parallel across the input port of the second BAW resonator pass-band filter circuit and a reference node of the second BAW resonator pass-band filter circuit or coupled in parallel between the output port of the second BAW resonator filter and the reference node, the first rejection-band shunt resonator having a first resonant frequency peak in a second rejection-band of frequencies that is greater than the second pass-band of frequencies. A switch can be configured to couple the input signal to the first rejection-band series resonator in a first state and configured to couple the input signal to the first rejection-band shunt resonator in a second state.

BRIEF DESCRIPTION OF THE DRAWINGS

In order to more fully understand the present invention, reference is made to the accompanying drawings. Understanding that these drawings are not to be considered limitations in the scope of the invention, the presently described embodiments and the presently understood best mode of the invention are described with additional detail through use of the accompanying drawings in which:

FIG. 1A is a simplified diagram illustrating an acoustic resonator device having topside interconnections according to an example of the present invention.

FIG. 1B is a simplified diagram illustrating an acoustic resonator device having bottom-side interconnections according to an example of the present invention.

FIG. 1C is a simplified diagram illustrating an acoustic resonator device having interposer/cap-free structure interconnections according to an example of the present invention.

FIG. 1D is a simplified diagram illustrating an acoustic resonator device having interposer/cap-free structure interconnections with a shared backside trench according to an example of the present invention.

FIGS. 2 and 3 are simplified diagrams illustrating steps for a method of manufacture for an acoustic resonator device according to an example of the present invention.

FIG. 4A is a simplified diagram illustrating a step for a method creating a topside micro-trench according to an example of the present invention.

FIGS. 4B and 4C are simplified diagrams illustrating alternative methods for conducting the method step of forming a topside micro-trench as described in FIG. 4A.

FIGS. 4D and 4E are simplified diagrams illustrating an alternative method for conducting the method step of forming a topside micro-trench as described in FIG. 4A.

FIGS. 5 to 8 are simplified diagrams illustrating steps for a method of manufacture for an acoustic resonator device according to an example of the present invention.

FIG. 9A is a simplified diagram illustrating a method step for forming backside trenches according to an example of the present invention.

FIGS. 9B and 9C are simplified diagrams illustrating an alternative method for conducting the method step of forming backside trenches, as described in FIG. 9A, and simultaneously singulating a seed substrate according to an embodiment of the present invention.

FIG. 10 is a simplified diagram illustrating a method step forming backside metallization and electrical interconnections between top and bottom sides of a resonator according to an example of the present invention.

FIGS. 11A and 11B are simplified diagrams illustrating alternative steps for a method of manufacture for an acoustic resonator device according to an example of the present invention.

FIGS. 12A to 12E are simplified diagrams illustrating steps for a method of manufacture for an acoustic resonator device using a blind via interposer according to an example of the present invention.

FIG. 13 is a simplified diagram illustrating a step for a method of manufacture for an acoustic resonator device according to an example of the present invention.

FIGS. 14A to 14G are simplified diagrams illustrating method steps for a cap wafer process for an acoustic resonator device according to an example of the present invention.

FIGS. 15A-15E are simplified diagrams illustrating method steps for making an acoustic resonator device with shared backside trench, which can be implemented in both interposer/cap and interposer free versions, according to examples of the present invention.

FIGS. 16A-16C through FIGS. 31A-31C are simplified diagrams illustrating various cross-sectional views of a single crystal acoustic resonator device and of method steps for a transfer process using a sacrificial layer for single crystal acoustic resonator devices according to an example of the present invention.

FIGS. 32A-32C through FIGS. 46A-46C are simplified diagrams illustrating various cross-sectional views of a single crystal acoustic resonator device and of method steps for a cavity bond transfer process for single crystal acoustic resonator devices according to an example of the present invention.

FIGS. 47A-47C though FIGS. 59A-59C are simplified diagrams illustrating various cross-sectional views of a single crystal acoustic resonator device and of method steps for a solidly mounted transfer process for single crystal acoustic resonator devices according to an example of the present invention.

FIG. 60 is a simplified diagram illustrating filter pass-band requirements in a radio frequency spectrum according to an example of the present invention.

FIG. 61 is a simplified diagram illustrating an overview of key markets that are applications for acoustic wave RF filters according to an example of the present invention.

FIG. 62 is a simplified diagram illustrating application areas for 5.2 GHz RF filters in Tri-Band Wi-Fi radios according to examples of the present invention.

FIGS. 63A-63C are simplified diagrams illustrating cross-sectional views of resonator devices according to various examples of the present invention.

FIGS. 64A-64C are simplified circuit diagrams illustrating representative lattice and ladder configurations for acoustic filter designs according to examples of the present invention.

FIGS. 65A-65B are simplified diagrams illustrating packing approaches according to various examples of the present invention.

FIG. 66 is a simplified diagram illustrating a packing approach according to an example of the present invention.

FIG. 67 is a simplified circuit diagram illustrating a 2-port BAW RF filter circuit according to an example of the present invention.

FIG. 68 is a simplified table of filter parameters according to an example of the present invention.

FIG. 69 is a simplified graph representing insertion loss over frequency according to an example of the present invention.

FIGS. 70-74 is a simplified circuit block diagram illustrating a front end module according to various examples of the present invention.

FIG. 75 is a schematic illustration of a BAW resonator filter including a BAW resonator pass-band filter ladder and first and second rejection-band series resonators in some embodiments according to the invention.

FIG. 76 is a graph illustrating anti-resonant frequencies of first and second rejection-band series resonators in the BAW resonator filter of FIG. 75 in some embodiments according to the invention.

FIG. 77 is a schematic illustration of a BAW resonator filter including a BAW resonator pass-band filter ladder and first and second rejection-band shunt resonators in some embodiments according to the invention.

FIG. 78 is a graph illustrating resonant frequencies of first and second rejection-band shunt resonators in the BAW resonator filter of FIG. 77 in some embodiments according to the invention.

FIG. 79 is a schematic illustration of a combined BAW resonator filter including a BAW resonator pass-band filter ladder with first and second rejection-band series resonators and a BAW resonator pass-band filter ladder with first and second rejection-band shunt resonators controlled by a switch in some embodiments according to the invention.

FIG. 80 is a schematic illustration of a BAW resonator filter including a BAW resonator pass-band filter lattice of FIG. 64A including first and second rejection-band series resonators in some embodiments according to the invention.

FIG. 81 is a schematic illustration of a BAW resonator filter including a BAW resonator pass-band filter lattice of FIG. 64B including first and second rejection-band series resonators in some embodiments according to the invention.

FIG. 82 is a graph representative of the BAW resonator filter response of FIGS. 80 and 81 including the anti-resonant frequencies of the first and second rejection-band series resonators in some embodiments according to the invention.

FIG. 83 is a schematic illustration of a BAW resonator filter including a BAW resonator pass-band filter lattice of FIG. 64A including first and second rejection-band shunt resonators in some embodiments according to the invention.

FIG. 84 is a schematic illustration of a BAW resonator filter including a BAW resonator pass-band filter lattice of FIG. 64B including first and second rejection-band shunt resonators in some embodiments according to the invention.

FIG. 85 is a graph representative of the BAW resonator filter response of FIGS. 83 and 84 including the anti-resonant frequencies of the first and second rejection-band shunt resonators in some embodiments according to the invention.

DETAILED DESCRIPTION OF EMBODIMENTS ACCORDING TO THE INVENTION

According to the present invention, techniques generally related to electronic devices are provided. More particularly, the present invention provides techniques related to a method of manufacture and structure for bulk acoustic wave resonator devices, single crystal resonator devices, single crystal filter and resonator devices, and the like. Merely by way of example, the invention has been applied to a single crystal resonator device for a communication device, mobile device, computing device, among others.

FIG. 1A is a simplified diagram illustrating an acoustic resonator device 101 having topside interconnections according to an example of the present invention. As shown, device 101 includes a thinned seed substrate 112 with an overlying single crystal piezoelectric layer 120, which has a micro-via 129. The micro-via 129 can include a topside micro-trench 121, a topside metal plug 146, a backside trench 114, and a backside metal plug 147. Although device 101 is depicted with a single micro-via 129, device 101 may have multiple micro-vias. A topside metal electrode 130 is formed overlying the piezoelectric layer 120. A top cap structure is bonded to the piezoelectric layer 120. This top cap structure includes an interposer substrate 119 with one or more through-vias 151 that are connected to one or more top bond pads 143, one or more bond pads 144, and topside metal 145 with topside metal plug 146. Solder balls 170 are electrically coupled to the one or more top bond pads 143.

The thinned substrate 112 has the first and second backside trenches 113, 114. A backside metal electrode 131 is formed underlying a portion of the thinned seed substrate 112, the first backside trench 113, and the topside metal electrode 130. The backside metal plug 147 is formed underlying a portion of the thinned seed substrate 112, the second backside trench 114, and the topside metal 145. This backside metal plug 147 is electrically coupled to the topside metal plug 146 and the backside metal electrode 131. A backside cap structure 161 is bonded to the thinned seed substrate 112, underlying the first and second backside trenches 113, 114. Further details relating to the method of manufacture of this device will be discussed starting from FIG. 2.

FIG. 1B is a simplified diagram illustrating an acoustic resonator device 102 having backside interconnections according to an example of the present invention. As shown, device 101 includes a thinned seed substrate 112 with an overlying piezoelectric layer 120, which has a micro-via 129. The micro-via 129 can include a topside micro-trench 121, a topside metal plug 146, a backside trench 114, and a backside metal plug 147. Although device 102 is depicted with a single micro-via 129, device 102 may have multiple micro-vias. A topside metal electrode 130 is formed overlying the piezoelectric layer 120. A top cap structure is bonded to the piezoelectric layer 120. This top cap structure 119 includes bond pads which are connected to one or more bond pads 144 and topside metal 145 on piezoelectric layer 120. The topside metal 145 includes a topside metal plug 146.

The thinned substrate 112 has the first and second backside trenches 113, 114. A backside metal electrode 131 is formed underlying a portion of the thinned seed substrate 112, the first backside trench 113, and the topside metal electrode 130. A backside metal plug 147 is formed underlying a portion of the thinned seed substrate 112, the second backside trench 114, and the topside metal plug 146. This backside metal plug 147 is electrically coupled to the topside metal plug 146. A backside cap structure 162 is bonded to the thinned seed substrate 112, underlying the first and second backside trenches. One or more backside bond pads (171, 172, 173) are formed within one or more portions of the backside cap structure 162. Solder balls 170 are electrically coupled to the one or more backside bond pads 171-173. Further details relating to the method of manufacture of this device will be discussed starting from FIG. 14A.

FIG. 1C is a simplified diagram illustrating an acoustic resonator device having interposer/cap-free structure interconnections according to an example of the present invention. As shown, device 103 includes a thinned seed substrate 112 with an overlying single crystal piezoelectric layer 120, which has a micro-via 129. The micro-via 129 can include a topside micro-trench 121, a topside metal plug 146, a backside trench 114, and a backside metal plug 147. Although device 103 is depicted with a single micro-via 129, device 103 may have multiple micro-vias. A topside metal electrode 130 is formed overlying the piezoelectric layer 120. The thinned substrate 112 has the first and second backside trenches 113, 114. A backside metal electrode 131 is formed underlying a portion of the thinned seed substrate 112, the first backside trench 113, and the topside metal electrode 130. A backside metal plug 147 is formed underlying a portion of the thinned seed substrate 112, the second backside trench 114, and the topside metal 145. This backside metal plug 147 is electrically coupled to the topside metal plug 146 and the backside metal electrode 131. Further details relating to the method of manufacture of this device will be discussed starting from FIG. 2.

FIG. 1D is a simplified diagram illustrating an acoustic resonator device having interposer/cap-free structure interconnections with a shared backside trench according to an example of the present invention. As shown, device 104 includes a thinned seed substrate 112 with an overlying single crystal piezoelectric layer 120, which has a micro-via 129. The micro-via 129 can include a topside micro-trench 121, a topside metal plug 146, and a backside metal 147. Although device 104 is depicted with a single micro-via 129, device 104 may have multiple micro-vias. A topside metal electrode 130 is formed overlying the piezoelectric layer 120. The thinned substrate 112 has a first backside trench 113. A backside metal electrode 131 is formed underlying a portion of the thinned seed substrate 112, the first backside trench 113, and the topside metal electrode 130. A backside metal 147 is formed underlying a portion of the thinned seed substrate 112, the second backside trench 114, and the topside metal 145. This backside metal 147 is electrically coupled to the topside metal plug 146 and the backside metal electrode 131. Further details relating to the method of manufacture of this device will be discussed starting from FIG. 2.

FIGS. 2 and 3 are simplified diagrams illustrating steps for a method of manufacture for an acoustic resonator device according to an example of the present invention. This method illustrates the process for fabricating an acoustic resonator device similar to that shown in FIG. 1A. FIG. 2 can represent a method step of providing a partially processed piezoelectric substrate. As shown, device 102 includes a seed substrate 110 with a piezoelectric layer 120 formed overlying. In a specific example, the seed substrate can include silicon, silicon carbide, aluminum oxide, or single crystal aluminum gallium nitride materials, or the like. The piezoelectric layer 120 can include a piezoelectric single crystal layer or a thin film piezoelectric single crystal layer.

FIG. 3 can represent a method step of forming a top side metallization or top resonator metal electrode 130. In a specific example, the topside metal electrode 130 can include a molybdenum, aluminum, ruthenium, or titanium material, or the like and combinations thereof. This layer can be deposited and patterned on top of the piezoelectric layer by a lift-off process, a wet etching process, a dry etching process, a metal printing process, a metal laminating process, or the like. The lift-off process can include a sequential process of lithographic patterning, metal deposition, and lift-off steps to produce the topside metal layer. The wet/dry etching processes can includes sequential processes of metal deposition, lithographic patterning, metal deposition, and metal etching steps to produce the topside metal layer. Those of ordinary skill in the art will recognize other variations, modifications, and alternatives.

FIG. 4A is a simplified diagram illustrating a step for a method of manufacture for an acoustic resonator device 401 according to an example of the present invention. This figure can represent a method step of forming one or more topside micro-trenches 121 within a portion of the piezoelectric layer 120. This topside micro-trench 121 can serve as the main interconnect junction between the top and bottom sides of the acoustic membrane, which will be developed in later method steps. In an example, the topside micro-trench 121 is extends all the way through the piezoelectric layer 120 and stops in the seed substrate 110. This topside micro-trench 121 can be formed through a dry etching process, a laser drilling process, or the like. FIGS. 4B and 4C describe these options in more detail.

FIGS. 4B and 4C are simplified diagrams illustrating alternative methods for conducting the method step as described in FIG. 4A. As shown, FIG. 4B represents a method step of using a laser drill, which can quickly and accurately form the topside micro-trench 121 in the piezoelectric layer 120. In an example, the laser drill can be used to form nominal 50 um holes, or holes between 10 um and 500 um in diameter, through the piezoelectric layer 120 and stop in the seed substrate 110 below the interface between layers 120 and 110. A protective layer 122 can be formed overlying the piezoelectric layer 120 and the topside metal electrode 130. This protective layer 122 can serve to protect the device from laser debris and to provide a mask for the etching of the topside micro-via 121. In a specific example, the laser drill can be an 11 W high power diode-pumped UV laser, or the like. This mask 122 can be subsequently removed before proceeding to other steps. The mask may also be omitted from the laser drilling process, and air flow can be used to remove laser debris.

FIG. 4C can represent a method step of using a dry etching process to form the topside micro-trench 121 in the piezoelectric layer 120. As shown, a lithographic masking layer 123 can be forming overlying the piezoelectric layer 120 and the topside metal electrode 130. The topside micro-trench 121 can be formed by exposure to plasma, or the like.

FIGS. 4D and 4E are simplified diagrams illustrating an alternative method for conducting the method step as described in FIG. 4A. These figures can represent the method step of manufacturing multiple acoustic resonator devices simultaneously. In FIG. 4D, two devices are shown on Die #1 and Die #2, respectively. FIG. 4E shows the process of forming a micro-via 121 on each of these dies while also etching a scribe line 124 or dicing line. In an example, the etching of the scribe line 124 singulates and relieves stress in the piezoelectric single crystal layer 120.

FIGS. 5 to 8 are simplified diagrams illustrating steps for a method of manufacture for an acoustic resonator device according to an example of the present invention. FIG. 5 can represent the method step of forming one or more bond pads 140 and forming a topside metal 141 electrically coupled to at least one of the bond pads 140. The topside metal 141 can include a topside metal plug 146 formed within the topside micro-trench 121. In a specific example, the topside metal plug 146 fills the topside micro-trench 121 to form a topside portion of a micro-via.

In an example, the bond pads 140 and the topside metal 141 can include a gold material or other interconnect metal material depending upon the application of the device. These metal materials can be formed by a lift-off process, a wet etching process, a dry etching process, a screen-printing process, an electroplating process, a metal printing process, or the like. In a specific example, the deposited metal materials can also serve as bond pads for a cap structure, which will be described below.

FIG. 6 can represent a method step for preparing the acoustic resonator device for bonding, which can be a hermetic bonding. As shown, a top cap structure is positioned above the partially processed acoustic resonator device as described in the previous figures. The top cap structure can be formed using an interposer substrate 119 in two configurations: fully processed interposer version 601 (through glass via) and partially processed interposer version 602 (blind via version). In the 601 version, the interposer substrate 119 includes through-via structures 151 that extend through the interposer substrate 119 and are electrically coupled to bottom bond pads 142 and top bond pads 143. In the 602 version, the interposer substrate 119 includes blind via structures 152 that only extend through a portion of the interposer substrate 119 from the bottom side. These blind via structures 152 are also electrically coupled to bottom bond pads 142. In a specific example, the interposer substrate can include a silicon, glass, smart-glass, or other like material.

FIG. 7 can represent a method step of bonding the top cap structure to the partially processed acoustic resonator device. As shown, the interposer substrate 119 is bonded to the piezoelectric layer by the bond pads (140, 142) and the topside metal 141, which are now denoted as bond pad 144 and topside metal 145. This bonding process can be done using a compression bond method or the like. FIG. 8 can represent a method step of thinning the seed substrate 110, which is now denoted as thinned seed substrate 111. This substrate thinning process can include grinding and etching processes or the like. In a specific example, this process can include a wafer backgrinding process followed by stress removal, which can involve dry etching, CMP polishing, or annealing processes.

FIG. 9A is a simplified diagram illustrating a step for a method of manufacture for an acoustic resonator device 901 according to an example of the present invention. FIG. 9A can represent a method step for forming backside trenches 113 and 114 to allow access to the piezoelectric layer from the backside of the thinned seed substrate 111. In an example, the first backside trench 113 can be formed within the thinned seed substrate 111 and underlying the topside metal electrode 130. The second backside trench 114 can be formed within the thinned seed substrate 111 and underlying the topside micro-trench 121 and topside metal plug 146. This substrate is now denoted thinned substrate 112. In a specific example, these trenches 113 and 114 can be formed using deep reactive ion etching (DRIE) processes, Bosch processes, or the like. The size, shape, and number of the trenches may vary with the design of the acoustic resonator device. In various examples, the first backside trench may be formed with a trench shape similar to a shape of the topside metal electrode or a shape of the backside metal electrode. The first backside trench may also be formed with a trench shape that is different from both a shape of the topside metal electrode and the backside metal electrode.

FIGS. 9B and 9C are simplified diagrams illustrating an alternative method for conducting the method step as described in FIG. 9A. Like FIGS. 4D and 4E, these figures can represent the method step of manufacturing multiple acoustic resonator devices simultaneously. In FIG. 9B, two devices with cap structures are shown on Die #1 and Die #2, respectively. FIG. 9C shows the process of forming backside trenches (113, 114) on each of these dies while also etching a scribe line 115 or dicing line. In an example, the etching of the scribe line 115 provides an optional way to singulate the backside wafer 112.

FIG. 10 is a simplified diagram illustrating a step for a method of manufacture for an acoustic resonator device 1000 according to an example of the present invention. This figure can represent a method step of forming a backside metal electrode 131 and a backside metal plug 147 within the backside trenches of the thinned seed substrate 112. In an example, the backside metal electrode 131 can be formed underlying one or more portions of the thinned substrate 112, within the first backside trench 113, and underlying the topside metal electrode 130. This process completes the resonator structure within the acoustic resonator device. The backside metal plug 147 can be formed underlying one or more portions of the thinned substrate 112, within the second backside trench 114, and underlying the topside micro-trench 121. The backside metal plug 147 can be electrically coupled to the topside metal plug 146 and the backside metal electrode 131. In a specific example, the backside metal electrode 130 can include a molybdenum, aluminum, ruthenium, or titanium material, or the like and combinations thereof. The backside metal plug can include a gold material, low resistivity interconnect metals, electrode metals, or the like. These layers can be deposited using the deposition methods described previously.

FIGS. 11A and 11B are simplified diagrams illustrating alternative steps for a method of manufacture for an acoustic resonator device according to an example of the present invention. These figures show methods of bonding a backside cap structure underlying the thinned seed substrate 112. In FIG. 11A, the backside cap structure is a dry film cap 161, which can include a permanent photo-imageable dry film such as a solder mask, polyimide, or the like. Bonding this cap structure can be cost-effective and reliable, but may not produce a hermetic seal. In FIG. 11B, the backside cap structure is a substrate 162, which can include a silicon, glass, or other like material. Bonding this substrate can provide a hermetic seal, but may cost more and require additional processes. Depending upon application, either of these backside cap structures can be bonded underlying the first and second backside vias.

FIGS. 12A to 12E are simplified diagrams illustrating steps for a method of manufacture for an acoustic resonator device according to an example of the present invention. More specifically, these figures describe additional steps for processing the blind via interposer “602” version of the top cap structure. FIG. 12A shows an acoustic resonator device 1201 with blind vias 152 in the top cap structure. In FIG. 12B, the interposer substrate 119 is thinned, which forms a thinned interposer substrate 118, to expose the blind vias 152. This thinning process can be a combination of a grinding process and etching process as described for the thinning of the seed substrate. In FIG. 12C, a redistribution layer (RDL) process and metallization process can be applied to create top cap bond pads 160 that are formed overlying the blind vias 152 and are electrically coupled to the blind vias 152. As shown in FIG. 12D, a ball grid array (BGA) process can be applied to form solder balls 170 overlying and electrically coupled to the top cap bond pads 160. This process leaves the acoustic resonator device ready for wire bonding 171, as shown in FIG. 12E.

FIG. 13 is a simplified diagram illustrating a step for a method of manufacture for an acoustic resonator device according to an example of the present invention. As shown, device 1300 includes two fully processed acoustic resonator devices that are ready to singulation to create separate devices. In an example, the die singulation process can be done using a wafer dicing saw process, a laser cut singulation process, or other processes and combinations thereof.

FIGS. 14A to 14G are simplified diagrams illustrating steps for a method of manufacture for an acoustic resonator device according to an example of the present invention. This method illustrates the process for fabricating an acoustic resonator device similar to that shown in FIG. 1B. The method for this example of an acoustic resonator can go through similar steps as described in FIGS. 1-5. FIG. 14A shows where this method differs from that described previously. Here, the top cap structure substrate 119 and only includes one layer of metallization with one or more bottom bond pads 142. Compared to FIG. 6, there are no via structures in the top cap structure because the interconnections will be formed on the bottom side of the acoustic resonator device.

FIGS. 14B to 14F depict method steps similar to those described in the first process flow. FIG. 14B can represent a method step of bonding the top cap structure to the piezoelectric layer 120 through the bond pads (140, 142) and the topside metal 141, now denoted as bond pads 144 and topside metal 145 with topside metal plug 146. FIG. 14C can represent a method step of thinning the seed substrate 110, which forms a thinned seed substrate 111, similar to that described in FIG. 8. FIG. 14D can represent a method step of forming first and second backside trenches, similar to that described in FIG. 9A. FIG. 14E can represent a method step of forming a backside metal electrode 131 and a backside metal plug 147, similar to that described in FIG. 10. FIG. 14F can represent a method step of bonding a backside cap structure 162, similar to that described in FIGS. 11A and 11B.

FIG. 14G shows another step that differs from the previously described process flow. Here, the backside bond pads 171, 172, and 173 are formed within the backside cap structure 162. In an example, these backside bond pads 171-173 can be formed through a masking, etching, and metal deposition processes similar to those used to form the other metal materials. A BGA process can be applied to form solder balls 170 in contact with these backside bond pads 171-173, which prepares the acoustic resonator device 1407 for wire bonding.

FIGS. 15A to 15E are simplified diagrams illustrating steps for a method of manufacture for an acoustic resonator device according to an example of the present invention. This method illustrates the process for fabricating an acoustic resonator device similar to that shown in FIG. 1B. The method for this example can go through similar steps as described in FIG. 1-5. FIG. 15A shows where this method differs from that described previously. A temporary carrier 218 with a layer of temporary adhesive 217 is attached to the substrate. In a specific example, the temporary carrier 218 can include a glass wafer, a silicon wafer, or other wafer and the like.

FIGS. 15B to 15F depict method steps similar to those described in the first process flow. FIG. 15B can represent a method step of thinning the seed substrate 110, which forms a thinned substrate 111, similar to that described in FIG. 8. In a specific example, the thinning of the seed substrate 110 can include a back side grinding process followed by a stress removal process. The stress removal process can include a dry etch, a Chemical Mechanical Planarization (CMP), and annealing processes.

FIG. 15C can represent a method step of forming a shared backside trench 113, similar to the techniques described in FIG. 9A. The main difference is that the shared backside trench is configured underlying both topside metal electrode 130, topside micro-trench 121, and topside metal plug 146. In an example, the shared backside trench 113 is a backside resonator cavity that can vary in size, shape (all possible geometric shapes), and side wall profile (tapered convex, tapered concave, or right angle). In a specific example, the forming of the shared backside trench 113 can include a litho-etch process, which can include a back-to-front alignment and dry etch of the backside substrate 111. The piezoelectric layer 120 can serve as an etch stop layer for the forming of the shared backside trench 113.

FIG. 15D can represent a method step of forming a backside metal electrode 131 and a backside metal 147, similar to that described in FIG. 10. In an example, the forming of the backside metal electrode 131 can include a deposition and patterning of metal materials within the shared backside trench 113. Here, the backside metal 131 serves as an electrode and the backside plug/connect metal 147 within the micro-via 121. The thickness, shape, and type of metal can vary as a function of the resonator/filter design. As an example, the backside electrode 131 and via plug metal 147 can be different metals. In a specific example, these backside metals 131, 147 can either be deposited and patterned on the surface of the piezoelectric layer 120 or rerouted to the backside of the substrate 112. In an example, the backside metal electrode may be patterned such that it is configured within the boundaries of the shared backside trench such that the backside metal electrode does not come in contact with one or more side-walls of the seed substrate created during the forming of the shared backside trench.

FIG. 15E can represent a method step of bonding a backside cap structure 162, similar to that described in FIGS. 11A and 11B, following a de-bonding of the temporary carrier 218 and cleaning of the topside of the device to remove the temporary adhesive 217. Those of ordinary skill in the art will recognize other variations, modifications, and alternatives of the methods steps described previously.

As used herein, the term “substrate” can mean the bulk substrate or can include overlying growth structures such as an aluminum, gallium, or ternary compound of aluminum and gallium and nitrogen containing epitaxial region, or functional regions, combinations, and the like.

One or more benefits are achieved over pre-existing techniques using the invention. In particular, the present device can be manufactured in a relatively simple and cost effective manner while using conventional materials and/or methods according to one of ordinary skill in the art. Using the present method, one can create a reliable single crystal based acoustic resonator using multiple ways of three-dimensional stacking through a wafer level process. Such filters or resonators can be implemented in an RF filter device, an RF filter system, or the like. Depending upon the embodiment, one or more of these benefits may be achieved. Of course, there can be other variations, modifications, and alternatives.

With 4G LTE and 5G growing more popular by the day, wireless data communication demands high performance RF filters with frequencies around 5 GHz and higher. Bulk acoustic wave resonators (BAWR), widely used in such filters operating at frequencies around 3 GHz and lower, are leading candidates for meeting such demands. Current bulk acoustic wave resonators use polycrystalline piezoelectric AlN thin films where each grain's c-axis is aligned perpendicular to the film's surface to allow high piezoelectric performance whereas the grains' a- or b-axis are randomly distributed. This peculiar grain distribution works well when the piezoelectric film's thickness is around 1 um and above, which is the perfect thickness for bulk acoustic wave (BAW) filters operating at frequencies ranging from 1 to 3 GHz. However, the quality of the polycrystalline piezoelectric films degrades quickly as the thicknesses decrease below around 0.5 um, which is required for resonators and filters operating at frequencies around 5 GHz and above.

Single crystalline or epitaxial piezoelectric thin films grown on compatible crystalline substrates exhibit good crystalline quality and high piezoelectric performance even down to very thin thicknesses, e.g., 0.4 um. The present invention provides manufacturing processes and structures for high quality bulk acoustic wave resonators with single crystalline or epitaxial piezoelectric thn films for high frequency BAW filter applications.

BAWRs require a piezoelectric material, e.g., AlN, in crystalline form, i.e., polycrystalline or single crystalline. The quality of the film heavy depends on the chemical, crystalline, or topographical quality of the layer on which the film is grown. In conventional BAWR processes (including film bulk acoustic resonator (FBAR) or solidly mounted resonator (SMR) geometry), the piezoelectric film is grown on a patterned bottom electrode, which is usually made of molybdenum (Mo), tungsten (W), or ruthenium (Ru). The surface geometry of the patterned bottom electrode significantly influences the crystalline orientation and crystalline quality of the piezoelectric film, requiring complicated modification of the structure.

Thus, the present invention uses single crystalline piezoelectric films and thin film transfer processes to produce a BAWR with enhanced ultimate quality factor and electro-mechanical coupling for RF filters. Such methods and structures facilitate methods of manufacturing and structures for RF filters using single crystalline or epitaxial piezoelectric films to meet the growing demands of contemporary data communication.

In an example, the present invention provides transfer structures and processes for acoustic resonator devices, which provides a flat, high-quality, single-crystal piezoelectric film for superior acoustic wave control and high Q in high frequency. As described above, polycrystalline piezoelectric layers limit Q in high frequency. Also, growing epitaxial piezoelectric layers on patterned electrodes affects the crystalline orientation of the piezoelectric layer, which limits the ability to have tight boundary control of the resulting resonators. Embodiments of the present invention, as further described below, can overcome these limitations and exhibit improved performance and cost-efficiency.

FIGS. 16A-16C through FIGS. 31A-31C illustrate a method of fabrication for an acoustic resonator device using a transfer structure with a sacrificial layer. In these figure series described below, the “A” figures show simplified diagrams illustrating top cross-sectional views of single crystal resonator devices according to various embodiments of the present invention. The “B” figures show simplified diagrams illustrating lengthwise cross-sectional views of the same devices in the “A” figures. Similarly, the “C” figures show simplified diagrams illustrating widthwise cross-sectional views of the same devices in the “A” figures. In some cases, certain features are omitted to highlight other features and the relationships between such features. Those of ordinary skill in the art will recognize variations, modifications, and alternatives to the examples shown in these figure series.

FIGS. 16A-16C are simplified diagrams illustrating various cross-sectional views of a single crystal acoustic resonator device and of method steps for a transfer process using a sacrificial layer for single crystal acoustic resonator devices according to an example of the present invention. As shown, these figures illustrate the method step of forming a piezoelectric film 1620 overlying a growth substrate 1610. In an example, the growth substrate 1610 can include silicon (S), silicon carbide (SiC), or other like materials. The piezoelectric film 1620 can be an epitaxial film including aluminum nitride (AlN), gallium nitride (GaN), or other like materials. Additionally, this piezoelectric substrate can be subjected to a thickness trim.

FIGS. 17A-17C are simplified diagrams illustrating various cross-sectional views of a single crystal acoustic resonator device and of method steps for a transfer process using a sacrificial layer for single crystal acoustic resonator devices according to an example of the present invention. As shown, these figures illustrate the method step of forming a first electrode 1710 overlying the surface region of the piezoelectric film 1620. In an example, the first electrode 1710 can include molybdenum (Mo), ruthenium (Ru), tungsten (W), or other like materials. In a specific example, the first electrode 1710 can be subjected to a dry etch with a slope. As an example, the slope can be about 60 degrees.

FIGS. 18A-18C are simplified diagrams illustrating various cross-sectional views of a single crystal acoustic resonator device and of method steps for a transfer process using a sacrificial layer for single crystal acoustic resonator devices according to an example of the present invention. As shown, these figures illustrate the method step of forming a first passivation layer 1810 overlying the first electrode 1710 and the piezoelectric film 1620. In an example, the first passivation layer 1810 can include silicon nitride (SiN), silicon oxide (SiOx), or other like materials. In a specific example, the first passivation layer 1810 can have a thickness ranging from about 50 nm to about 100 nm.

FIGS. 19A-19C are simplified diagrams illustrating various cross-sectional views of a single crystal acoustic resonator device and of method steps for a transfer process using a sacrificial layer for single crystal acoustic resonator devices according to an example of the present invention. As shown, these figures illustrate the method step of forming a sacrificial layer 1910 overlying a portion of the first electrode 1810 and a portion of the piezoelectric film 1620. In an example, the sacrificial layer 1910 can include polycrystalline silicon (poly-Si), amorphous silicon (a-Si), or other like materials. In a specific example, this sacrificial layer 1910 can be subjected to a dry etch with a slope and be deposited with a thickness of about 1 um. Further, phosphorous doped SiO.sub.2 (PSG) can be used as the sacrificial layer with different combinations of support layer (e.g., SiNx).

FIGS. 20A-20C are simplified diagrams illustrating various cross-sectional views of a single crystal acoustic resonator device and of method steps for a transfer process using a sacrificial layer for single crystal acoustic resonator devices according to an example of the present invention. As shown, these figures illustrate the method step of forming a support layer 2010 overlying the sacrificial layer 1910, the first electrode 1710, and the piezoelectric film 1620. In an example, the support layer 2010 can include silicon dioxide (SiO.sub.2), silicon nitride (SiN), or other like materials. In a specific example, this support layer 2010 can be deposited with a thickness of about 2-3 um. As described above, other support layers (e.g., SiNx) can be used in the case of a PSG sacrificial layer.

FIGS. 21A-21C are simplified diagrams illustrating various cross-sectional views of a single crystal acoustic resonator device and of method steps for a transfer process using a sacrificial layer for single crystal acoustic resonator devices according to an example of the present invention. As shown, these figures illustrate the method step of polishing the support layer 2010 to form a polished support layer 2011. In an example, the polishing process can include a chemical-mechanical planarization process or the like.

FIGS. 22A-22C are simplified diagrams illustrating various cross-sectional views of a single crystal acoustic resonator device and of method steps for a transfer process using a sacrificial layer for single crystal acoustic resonator devices according to an example of the present invention. As shown, these figures illustrate flipping the device and physically coupling overlying the support layer 2011 overlying a bond substrate 2210. In an example, the bond substrate 2210 can include a bonding support layer 2220 (SiO.sub.2 or like material) overlying a substrate having silicon (Si), sapphire (Al.sub.20.sub.3), silicon dioxide (SiO.sub.2), silicon carbide (SiC), or other like materials. In a specific embodiment, the bonding support layer 2220 of the bond substrate 2210 is physically coupled to the polished support layer 2011. Further, the physical coupling process can include a room temperature bonding process following by a 300 degree Celsius annealing process.

FIGS. 23A-23C are simplified diagrams illustrating various cross-sectional views of a single crystal acoustic resonator device and of method steps for a transfer process using a sacrificial layer for single crystal acoustic resonator devices according to an example of the present invention. As shown, these figures illustrate the method step of removing the growth substrate 1610 or otherwise the transfer of the piezoelectric film 1620. In an example, the removal process can include a grinding process, a blanket etching process, a film transfer process, an ion implantation transfer process, a laser crack transfer process, or the like and combinations thereof.

FIGS. 24A-24C are simplified diagrams illustrating various cross-sectional views of a single crystal acoustic resonator device and of method steps for a transfer process using a sacrificial layer for single crystal acoustic resonator devices according to an example of the present invention. As shown, these figures illustrate the method step of forming an electrode contact via 2410 within the piezoelectric film 1620 (becoming piezoelectric film 1621) overlying the first electrode 1710 and forming one or more release holes 2420 within the piezoelectric film 1620 and the first passivation layer 1810 overlying the sacrificial layer 1910. The via forming processes can include various types of etching processes.

FIGS. 25A-25C are simplified diagrams illustrating various cross-sectional views of a single crystal acoustic resonator device and of method steps for a transfer process using a sacrificial layer for single crystal acoustic resonator devices according to an example of the present invention. As shown, these figures illustrate the method step of forming a second electrode 2510 overlying the piezoelectric film 1621. In an example, the formation of the second electrode 2510 includes depositing molybdenum (Mo), ruthenium (Ru), tungsten (W), or other like materials; and then etching the second electrode 2510 to form an electrode cavity 2511 and to remove portion 2511 from the second electrode to form a top metal 2520. Further, the top metal 2520 is physically coupled to the first electrode 1720 through electrode contact via 2410.

FIGS. 26A-26C are simplified diagrams illustrating various cross-sectional views of a single crystal acoustic resonator device and of method steps for a transfer process using a sacrificial layer for single crystal acoustic resonator devices according to an example of the present invention. As shown, these figures illustrate the method step of forming a first contact metal 2610 overlying a portion of the second electrode 2510 and a portion of the piezoelectric film 1621, and forming a second contact metal 2611 overlying a portion of the top metal 2520 and a portion of the piezoelectric film 1621. In an example, the first and second contact metals can include gold (Au), aluminum (Al), copper (Cu), nickel (Ni), aluminum bronze (AlCu), or related alloys of these materials or other like materials.

FIGS. 27A-27C are simplified diagrams illustrating various cross-sectional views of a single crystal acoustic resonator device and of method steps for a transfer process using a sacrificial layer for single crystal acoustic resonator devices according to an example of the present invention. As shown, these figures illustrate the method step of forming a second passivation layer 2710 overlying the second electrode 2510, the top metal 2520, and the piezoelectric film 1621. In an example, the second passivation layer 2710 can include silicon nitride (SiN), silicon oxide (SiOx), or other like materials. In a specific example, the second passivation layer 2710 can have a thickness ranging from about 50 nm to about 100 nm.

FIGS. 28A-28C are simplified diagrams illustrating various cross-sectional views of a single crystal acoustic resonator device and of method steps for a transfer process using a sacrificial layer for single crystal acoustic resonator devices according to an example of the present invention. As shown, these figures illustrate the method step of removing the sacrificial layer 1910 to form an air cavity 2810. In an example, the removal process can include a poly-Si etch or an a-Si etch, or the like.

FIGS. 29A-29C are simplified diagrams illustrating various cross-sectional views of a single crystal acoustic resonator device and of method steps for a transfer process using a sacrificial layer for single crystal acoustic resonator devices according to another example of the present invention. As shown, these figures illustrate the method step of processing the second electrode 2510 and the top metal 2520 to form a processed second electrode 2910 and a processed top metal 2920. This step can follow the formation of second electrode 2510 and top metal 2520. In an example, the processing of these two components includes depositing molybdenum (Mo), ruthenium (Ru), tungsten (W), or other like materials; and then etching (e.g., dry etch or the like) this material to form the processed second electrode 2910 with an electrode cavity 2912 and the processed top metal 2920. The processed top metal 2920 remains separated from the processed second electrode 2910 by the removal of portion 2911. In a specific example, the processed second electrode 2910 is characterized by the addition of an energy confinement structure configured on the processed second electrode 2910 to increase Q.

FIGS. 30A-30C are simplified diagrams illustrating various cross-sectional views of a single crystal acoustic resonator device and of method steps for a transfer process using a sacrificial layer for single crystal acoustic resonator devices according to another example of the present invention. As shown, these figures illustrate the method step of processing the first electrode 1710 to form a processed first electrode 2310. This step can follow the formation of first electrode 1710. In an example, the processing of these two components includes depositing molybdenum (Mo), ruthenium (Ru), tungsten (W), or other like materials; and then etching (e.g., dry etch or the like) this material to form the processed first electrode 3010 with an electrode cavity, similar to the processed second electrode 2910. Air cavity 2811 shows the change in cavity shape due to the processed first electrode 3010. In a specific example, the processed first electrode 3010 is characterized by the addition of an energy confinement structure configured on the processed second electrode 3010 to increase Q.

FIGS. 31A-31C are simplified diagrams illustrating various cross-sectional views of a single crystal acoustic resonator device and of method steps for a transfer process using a sacrificial layer for single crystal acoustic resonator devices according to another example of the present invention. As shown, these figures illustrate the method step of processing the first electrode 1710, to form a processed first electrode 2310, and the second electrode 2510/top metal 2520 to form a processed second electrode 2910/processed top metal 2920. These steps can follow the formation of each respective electrode, as described for FIGS. 29A-29C and 30A-30C. Those of ordinary skill in the art will recognize other variations, modifications, and alternatives.

FIGS. 32A-32C through FIGS. 46A-46C illustrate a method of fabrication for an acoustic resonator device using a transfer structure without sacrificial layer. In these figure series described below, the “A” figures show simplified diagrams illustrating top cross-sectional views of single crystal resonator devices according to various embodiments of the present invention. The “B” figures show simplified diagrams illustrating lengthwise cross-sectional views of the same devices in the “A” figures. Similarly, the “C” figures show simplified diagrams illustrating widthwise cross-sectional views of the same devices in the “A” figures. In some cases, certain features are omitted to highlight other features and the relationships between such features. Those of ordinary skill in the art will recognize variations, modifications, and alternatives to the examples shown in these figure series.

FIGS. 32A-32C are simplified diagrams illustrating various cross-sectional views of a single crystal acoustic resonator device and of method steps for a transfer process for single crystal acoustic resonator devices according to an example of the present invention. As shown, these figures illustrate the method step of forming a piezoelectric film 3220 overlying a growth substrate 3210. In an example, the growth substrate 3210 can include silicon (S), silicon carbide (SiC), or other like materials. The piezoelectric film 3220 can be an epitaxial film including aluminum nitride (AlN), gallium nitride (GaN), or other like materials. Additionally, this piezoelectric substrate can be subjected to a thickness trim.

FIGS. 33A-33C are simplified diagrams illustrating various cross-sectional views of a single crystal acoustic resonator device and of method steps for a transfer process for single crystal acoustic resonator devices according to an example of the present invention. As shown, these figures illustrate the method step of forming a first electrode 3310 overlying the surface region of the piezoelectric film 3220. In an example, the first electrode 3310 can include molybdenum (Mo), ruthenium (Ru), tungsten (W), or other like materials. In a specific example, the first electrode 3310 can be subjected to a dry etch with a slope. As an example, the slope can be about 60 degrees.

FIGS. 34A-34C are simplified diagrams illustrating various cross-sectional views of a single crystal acoustic resonator device and of method steps for a transfer process for single crystal acoustic resonator devices according to an example of the present invention. As shown, these figures illustrate the method step of forming a first passivation layer 3410 overlying the first electrode 3310 and the piezoelectric film 3220. In an example, the first passivation layer 3410 can include silicon nitride (SiN), silicon oxide (SiOx), or other like materials. In a specific example, the first passivation layer 3410 can have a thickness ranging from about 50 nm to about 100 nm.

FIGS. 35A-35C are simplified diagrams illustrating various cross-sectional views of a single crystal acoustic resonator device and of method steps for a transfer process for single crystal acoustic resonator devices according to an example of the present invention. As shown, these figures illustrate the method step of forming a support layer 3510 overlying the first electrode 3310, and the piezoelectric film 3220. In an example, the support layer 3510 can include silicon dioxide (SiO.sub.2), silicon nitride (SiN), or other like materials. In a specific example, this support layer 3510 can be deposited with a thickness of about 2-3 um. As described above, other support layers (e.g., SiNx) can be used in the case of a PSG sacrificial layer.

FIGS. 36A-36C are simplified diagrams illustrating various cross-sectional views of a single crystal acoustic resonator device and of method steps for a transfer process for single crystal acoustic resonator devices according to an example of the present invention. As shown, these figures illustrate the optional method step of processing the support layer 3510 (to form support layer 3511) in region 3610. In an example, the processing can include a partial etch of the support layer 3510 to create a flat bond surface. In a specific example, the processing can include a cavity region. In other examples, this step can be replaced with a polishing process such as a chemical-mechanical planarization process or the like.

FIGS. 37A-37C are simplified diagrams illustrating various cross-sectional views of a single crystal acoustic resonator device and of method steps for a transfer process for single crystal acoustic resonator devices according to an example of the present invention. As shown, these figures illustrate the method step of forming an air cavity 3710 within a portion of the support layer 3511 (to form support layer 3512). In an example, the cavity formation can include an etching process that stops at the first passivation layer 3410.

FIGS. 38A-38C are simplified diagrams illustrating various cross-sectional views of a single crystal acoustic resonator device and of method steps for a transfer process for single crystal acoustic resonator devices according to an example of the present invention. As shown, these figures illustrate the method step of forming one or more cavity vent holes 3810 within a portion of the piezoelectric film 3220 through the first passivation layer 3410. In an example, the cavity vent holes 3810 connect to the air cavity 3710.

FIGS. 39A-39C are simplified diagrams illustrating various cross-sectional views of a single crystal acoustic resonator device and of method steps for a transfer process for single crystal acoustic resonator devices according to an example of the present invention. As shown, these figures illustrate flipping the device and physically coupling overlying the support layer 3512 overlying a bond substrate 3910. In an example, the bond substrate 3910 can include a bonding support layer 3920 (SiO.sub.2 or like material) overlying a substrate having silicon (Si), sapphire (Al.sub.20.sub.3), silicon dioxide (SiO.sub.2), silicon carbide (SiC), or other like materials. In a specific embodiment, the bonding support layer 3920 of the bond substrate 3910 is physically coupled to the polished support layer 3512. Further, the physical coupling process can include a room temperature bonding process following by a 300 degree Celsius annealing process.

FIGS. 40A-40C are simplified diagrams illustrating various cross-sectional views of a single crystal acoustic resonator device and of method steps for a transfer process for single crystal acoustic resonator devices according to an example of the present invention. As shown, these figures illustrate the method step of removing the growth substrate 3210 or otherwise the transfer of the piezoelectric film 3220. In an example, the removal process can include a grinding process, a blanket etching process, a film transfer process, an ion implantation transfer process, a laser crack transfer process, or the like and combinations thereof.

FIGS. 41A-41C are simplified diagrams illustrating various cross-sectional views of a single crystal acoustic resonator device and of method steps for a transfer process for single crystal acoustic resonator devices according to an example of the present invention. As shown, these figures illustrate the method step of forming an electrode contact via 4110 within the piezoelectric film 3220 overlying the first electrode 3310. The via forming processes can include various types of etching processes.

FIGS. 42A-42C are simplified diagrams illustrating various cross-sectional views of a single crystal acoustic resonator device and of method steps for a transfer process for single crystal acoustic resonator devices according to an example of the present invention. As shown, these figures illustrate the method step of forming a second electrode 4210 overlying the piezoelectric film 3220. In an example, the formation of the second electrode 4210 includes depositing molybdenum (Mo), ruthenium (Ru), tungsten (W), or other like materials; and then etching the second electrode 4210 to form an electrode cavity 4211 and to remove portion 4211 from the second electrode to form a top metal 4220. Further, the top metal 4220 is physically coupled to the first electrode 3310 through electrode contact via 4110.

FIGS. 43A-43C are simplified diagrams illustrating various cross-sectional views of a single crystal acoustic resonator device and of method steps for a transfer process for single crystal acoustic resonator devices according to an example of the present invention. As shown, these figures illustrate the method step of forming a first contact metal 4310 overlying a portion of the second electrode 4210 and a portion of the piezoelectric film 3220, and forming a second contact metal 4311 overlying a portion of the top metal 4220 and a portion of the piezoelectric film 3220. In an example, the first and second contact metals can include gold (Au), aluminum (Al), copper (Cu), nickel (Ni), aluminum bronze (AlCu), or other like materials. This figure also shows the method step of forming a second passivation layer 4320 overlying the second electrode 4210, the top metal 4220, and the piezoelectric film 3220. In an example, the second passivation layer 4320 can include silicon nitride (SiN), silicon oxide (SiOx), or other like materials. In a specific example, the second passivation layer 4320 can have a thickness ranging from about 50 nm to about 100 nm.

FIGS. 44A-44C are simplified diagrams illustrating various cross-sectional views of a single crystal acoustic resonator device and of method steps for a transfer process for single crystal acoustic resonator devices according to another example of the present invention. As shown, these figures illustrate the method step of processing the second electrode 4210 and the top metal 4220 to form a processed second electrode 4410 and a processed top metal 4420. This step can follow the formation of second electrode 4210 and top metal 4220. In an example, the processing of these two components includes depositing molybdenum (Mo), ruthenium (Ru), tungsten (W), or other like materials; and then etching (e.g., dry etch or the like) this material to form the processed second electrode 4410 with an electrode cavity 4412 and the processed top metal 4420. The processed top metal 4420 remains separated from the processed second electrode 4410 by the removal of portion 4411. In a specific example, the processed second electrode 4410 is characterized by the addition of an energy confinement structure configured on the processed second electrode 4410 to increase Q.

FIGS. 45A-45C are simplified diagrams illustrating various cross-sectional views of a single crystal acoustic resonator device and of method steps for a transfer process using a sacrificial layer for single crystal acoustic resonator devices according to another example of the present invention. As shown, these figures illustrate the method step of processing the first electrode 3310 to form a processed first electrode 4510. This step can follow the formation of first electrode 3310. In an example, the processing of these two components includes depositing molybdenum (Mo), ruthenium (Ru), tungsten (W), or other like materials; and then etching (e.g., dry etch or the like) this material to form the processed first electrode 4510 with an electrode cavity, similar to the processed second electrode 4410. Air cavity 3711 shows the change in cavity shape due to the processed first electrode 4510. In a specific example, the processed first electrode 4510 is characterized by the addition of an energy confinement structure configured on the processed second electrode 4510 to increase Q.

FIGS. 46A-46C are simplified diagrams illustrating various cross-sectional views of a single crystal acoustic resonator device and of method steps for a transfer process using a sacrificial layer for single crystal acoustic resonator devices according to another example of the present invention. As shown, these figures illustrate the method step of processing the first electrode 3310, to form a processed first electrode 4510, and the second electrode 4210/top metal 4220 to form a processed second electrode 4410/processed top metal 4420. These steps can follow the formation of each respective electrode, as described for FIGS. 44A-44C and 45A-45C. Those of ordinary skill in the art will recognize other variations, modifications, and alternatives.

FIGS. 47A-47C through FIGS. 59A-59C illustrate a method of fabrication for an acoustic resonator device using a transfer structure with a multilayer mirror structure. In these figure series described below, the “A” figures show simplified diagrams illustrating top cross-sectional views of single crystal resonator devices according to various embodiments of the present invention. The “B” figures show simplified diagrams illustrating lengthwise cross-sectional views of the same devices in the “A” figures. Similarly, the “C” figures show simplified diagrams illustrating widthwise cross-sectional views of the same devices in the “A” figures. In some cases, certain features are omitted to highlight other features and the relationships between such features. Those of ordinary skill in the art will recognize variations, modifications, and alternatives to the examples shown in these figure series.

FIGS. 47A-47C are simplified diagrams illustrating various cross-sectional views of a single crystal acoustic resonator device and of method steps for a transfer process with a multilayer mirror for single crystal acoustic resonator devices according to an example of the present invention. As shown, these figures illustrate the method step of forming a piezoelectric film 4720 overlying a growth substrate 4710. In an example, the growth substrate 4710 can include silicon (S), silicon carbide (SiC), or other like materials. The piezoelectric film 4720 can be an epitaxial film including aluminum nitride (AlN), gallium nitride (GaN), or other like materials. Additionally, this piezoelectric substrate can be subjected to a thickness trim.

FIGS. 48A-48C are simplified diagrams illustrating various cross-sectional views of a single crystal acoustic resonator device and of method steps for a transfer process with a multilayer mirror for single crystal acoustic resonator devices according to an example of the present invention. As shown, these figures illustrate the method step of forming a first electrode 4810 overlying the surface region of the piezoelectric film 4720. In an example, the first electrode 4810 can include molybdenum (Mo), ruthenium (Ru), tungsten (W), or other like materials. In a specific example, the first electrode 4810 can be subjected to a dry etch with a slope. As an example, the slope can be about 60 degrees.

FIGS. 49A-49C are simplified diagrams illustrating various cross-sectional views of a single crystal acoustic resonator device and of method steps for a transfer process with a multilayer mirror for single crystal acoustic resonator devices according to an example of the present invention. As shown, these figures illustrate the method step of forming a multilayer mirror or reflector structure. In an example, the multilayer mirror includes at least one pair of layers with a low impedance layer 4910 and a high impedance layer 4920. In FIGS. 49A-49C, two pairs of low/high impedance layers are shown (low: 4910 and 4911; high: 4920 and 4921). In an example, the mirror/reflector area can be larger than the resonator area and can encompass the resonator area. In a specific embodiment, each layer thickness is about ¼ of the wavelength of an acoustic wave at a targeting frequency. The layers can be deposited in sequence and be etched afterwards, or each layer can be deposited and etched individually. In another example, the first electrode 4810 can be patterned after the mirror structure is patterned.

FIGS. 50A-50C are simplified diagrams illustrating various cross-sectional views of a single crystal acoustic resonator device and of method steps for a transfer process with a multilayer mirror for single crystal acoustic resonator devices according to an example of the present invention. As shown, these figures illustrate the method step of forming a support layer 5010 overlying the mirror structure (layers 4910, 4911, 4920, and 4921), the first electrode 4810, and the piezoelectric film 4720. In an example, the support layer 5010 can include silicon dioxide (SiO.sub.2), silicon nitride (SiN), or other like materials. In a specific example, this support layer 5010 can be deposited with a thickness of about 2-3 um. As described above, other support layers (e.g., SiNx) can be used.

FIGS. 51A-51C are simplified diagrams illustrating various cross-sectional views of a single crystal acoustic resonator device and of method steps for a transfer process with a multilayer mirror for single crystal acoustic resonator devices according to an example of the present invention. As shown, these figures illustrate the method step of polishing the support layer 5010 to form a polished support layer 5011. In an example, the polishing process can include a chemical-mechanical planarization process or the like.

FIGS. 52A-52C are simplified diagrams illustrating various cross-sectional views of a single crystal acoustic resonator device and of method steps for a transfer process with a multilayer mirror for single crystal acoustic resonator devices according to an example of the present invention. As shown, these figures illustrate flipping the device and physically coupling overlying the support layer 5011 overlying a bond substrate 5210. In an example, the bond substrate 5210 can include a bonding support layer 5220 (SiO.sub.2 or like material) overlying a substrate having silicon (Si), sapphire (Al.sub.20.sub.3), silicon dioxide (SiO.sub.2), silicon carbide (SiC), or other like materials. In a specific embodiment, the bonding support layer 5220 of the bond substrate 5210 is physically coupled to the polished support layer 5011. Further, the physical coupling process can include a room temperature bonding process following by a 300 degree Celsius annealing process.

FIGS. 53A-53C are simplified diagrams illustrating various cross-sectional views of a single crystal acoustic resonator device and of method steps for a transfer process with a multilayer mirror for single crystal acoustic resonator devices according to an example of the present invention. As shown, these figures illustrate the method step of removing the growth substrate 4710 or otherwise the transfer of the piezoelectric film 4720. In an example, the removal process can include a grinding process, a blanket etching process, a film transfer process, an ion implantation transfer process, a laser crack transfer process, or the like and combinations thereof.

FIGS. 54A-54C are simplified diagrams illustrating various cross-sectional views of a single crystal acoustic resonator device and of method steps for a transfer process with a multilayer mirror for single crystal acoustic resonator devices according to an example of the present invention. As shown, these figures illustrate the method step of forming an electrode contact via 5410 within the piezoelectric film 4720 overlying the first electrode 4810. The via forming processes can include various types of etching processes.

FIGS. 55A-55C are simplified diagrams illustrating various cross-sectional views of a single crystal acoustic resonator device and of method steps for a transfer process with a multilayer mirror for single crystal acoustic resonator devices according to an example of the present invention. As shown, these figures illustrate the method step of forming a second electrode 5510 overlying the piezoelectric film 4720. In an example, the formation of the second electrode 5510 includes depositing molybdenum (Mo), ruthenium (Ru), tungsten (W), or other like materials; and then etching the second electrode 5510 to form an electrode cavity 5511 and to remove portion 5511 from the second electrode to form a top metal 5520. Further, the top metal 5520 is physically coupled to the first electrode 5520 through electrode contact via 5410.

FIGS. 56A-56C are simplified diagrams illustrating various cross-sectional views of a single crystal acoustic resonator device and of method steps for a transfer process with a multilayer mirror for single crystal acoustic resonator devices according to an example of the present invention. As shown, these figures illustrate the method step of forming a first contact metal 5610 overlying a portion of the second electrode 5510 and a portion of the piezoelectric film 4720, and forming a second contact metal 5611 overlying a portion of the top metal 5520 and a portion of the piezoelectric film 4720. In an example, the first and second contact metals can include gold (Au), aluminum (Al), copper (Cu), nickel (Ni), aluminum bronze (AlCu), or other like materials. This figure also shows the method step of forming a second passivation layer 5620 overlying the second electrode 5510, the top metal 5520, and the piezoelectric film 4720. In an example, the second passivation layer 5620 can include silicon nitride (SiN), silicon oxide (SiOx), or other like materials. In a specific example, the second passivation layer 5620 can have a thickness ranging from about 50 nm to about 100 nm.

FIGS. 57A-57C are simplified diagrams illustrating various cross-sectional views of a single crystal acoustic resonator device and of method steps for a transfer process with a multilayer mirror for single crystal acoustic resonator devices according to another example of the present invention. As shown, these figures illustrate the method step of processing the second electrode 5510 and the top metal 5520 to form a processed second electrode 5710 and a processed top metal 5720. This step can follow the formation of second electrode 5710 and top metal 5720. In an example, the processing of these two components includes depositing molybdenum (Mo), ruthenium (Ru), tungsten (W), or other like materials; and then etching (e.g., dry etch or the like) this material to form the processed second electrode 5410 with an electrode cavity 5712 and the processed top metal 5720. The processed top metal 5720 remains separated from the processed second electrode 5710 by the removal of portion 5711. In a specific example, this processing gives the second electrode and the top metal greater thickness while creating the electrode cavity 5712. In a specific example, the processed second electrode 5710 is characterized by the addition of an energy confinement structure configured on the processed second electrode 5710 to increase Q.

FIGS. 58A-58C are simplified diagrams illustrating various cross-sectional views of a single crystal acoustic resonator device and of method steps for a transfer process with a multilayer mirror for single crystal acoustic resonator devices according to another example of the present invention. As shown, these figures illustrate the method step of processing the first electrode 4810 to form a processed first electrode 5810. This step can follow the formation of first electrode 4810. In an example, the processing of these two components includes depositing molybdenum (Mo), ruthenium (Ru), tungsten (W), or other like materials; and then etching (e.g., dry etch or the like) this material to form the processed first electrode 5810 with an electrode cavity, similar to the processed second electrode 5710. Compared to the two previous examples, there is no air cavity. In a specific example, the processed first electrode 5810 is characterized by the addition of an energy confinement structure configured on the processed second electrode 5810 to increase Q.

FIGS. 59A-59C are simplified diagrams illustrating various cross-sectional views of a single crystal acoustic resonator device and of method steps for a transfer process with a multilayer mirror for single crystal acoustic resonator devices according to another example of the present invention. As shown, these figures illustrate the method step of processing the first electrode 4810, to form a processed first electrode 5810, and the second electrode 5510/top metal 5520 to form a processed second electrode 5710/processed top metal 5720. These steps can follow the formation of each respective electrode, as described for FIGS. 57A-57C and 58A-58C. Those of ordinary skill in the art will recognize other variations, modifications, and alternatives.

In each of the preceding examples relating to transfer processes, energy confinement structures can be formed on the first electrode, second electrode, or both. In an example, these energy confinement structures are mass loaded areas surrounding the resonator area. The resonator area is the area where the first electrode, the piezoelectric layer, and the second electrode overlap. The larger mass load in the energy confinement structures lowers a cut-off frequency of the resonator. The cut-off frequency is the lower or upper limit of the frequency at which the acoustic wave can propagate in a direction parallel to the surface of the piezoelectric film. Therefore, the cut-off frequency is the resonance frequency in which the wave is travelling along the thickness direction and thus is determined by the total stack structure of the resonator along the vertical direction. In piezoelectric films (e.g., AlN), acoustic waves with lower frequency than the cut-off frequency can propagate in a parallel direction along the surface of the film, i.e., the acoustic wave exhibits a high-band-cut-off type dispersion characteristic. In this case, the mass loaded area surrounding the resonator provides a barrier preventing the acoustic wave from propagating outside the resonator. By doing so, this feature increases the quality factor of the resonator and improves the performance of the resonator and, consequently, the filter.

In addition, the top single crystalline piezoelectric layer can be replaced by a polycrystalline piezoelectric film. In such films, the lower part that is close to the interface with the substrate has poor crystalline quality with smaller grain sizes and a wider distribution of the piezoelectric polarization orientation than the upper part of the film close to the surface. This is due to the polycrystalline growth of the piezoelectric film, i.e., the nucleation and initial film have random crystalline orientations. Considering AlN as a piezoelectric material, the growth rate along the c-axis or the polarization orientation is higher than other crystalline orientations that increase the proportion of the grains with the c-axis perpendicular to the growth surface as the film grows thicker. In a typical polycrystalline AlN film with about a 1 um thickness, the upper part of the film close to the surface has better crystalline quality and better alignment in terms of piezoelectric polarization. By using the thin film transfer process contemplated in the present invention, it is possible to use the upper portion of the polycrystalline film in high frequency BAW resonators with very thin piezoelectric films. This can be done by removing a portion of the piezoelectric layer during the growth substrate removal process. Of course, there can be other variations, modifications, and alternatives.

In an example, the present invention provides a high-performance, ultra-small pass-band Bulk Acoustic Wave (BAW) Radio Frequency (RF) Filter for use in 5.2 GHz Wi-Fi applications covering U-NII-1 plus U-NII-2A bands.

FIG. 60 is a simplified diagram illustrating filter pass-band requirements in a radio frequency spectrum according to an example of the present invention. As shown, the frequency spectrum 6000 shows a range from 3.0 GHz to 6.0 GHz. Here, a first application band 6010 (3.3 GHz-4.2 GHz) is configured for 5G applications. This band includes a 5G sub-band 6011 (3.3 GHz-3.8 GHz), which includes further LTE sub-bands 6012 (3.4 GHz-3.6 GHz), 6013 (3.6 GHz-3.8 GHz), and 6014 (3.55 GHz-3.7 GHz). A second application band 6020 (4.4 GHz-5.0 GHz) includes a sub-band 6021 for China specific applications. A third application band 6030 includes a UNII-1 band 6031 (5.15 GHz-5.25 GHz) and a UNII-2A band 6032 (5.25 GHz 5.33 GHz). An LTE band 6033 overlaps the same frequency range as the UNII-1 band 6031. Finally, a fourth application band 6040 includes a UNII-2C band 6041 (5.490 GHz-5.735 GHz), a UNII-3 band 6042 (5.735 GHz-5.85 GHz), and a UNII-4 band 6043 (5.85 GHz-5.925 GHz). An LTE band 6044 shares the same frequency range as the UNII-2C band 6041, while a sub-band 6045 overlaps the same frequency range as the UNII-4 band 6043 and an LTE band 6046 overlaps a smaller subsection of the same frequency range (5.855 GHz-5.925 GHz). Those of ordinary skill in the art will recognize other variations, modifications, and alternatives.

In an embodiment, the present filter utilizes single crystal BAW technology as described in the previous figures. This filter provides low insertion loss and meets the stringent rejection requirements enabling coexistence with U-NII-2C and U-NII-3 bands. The high-power rating satisfies the demanding power requirements of the latest Wi-Fi standards.

FIG. 61 is a simplified diagram illustrating an overview of key markets that are applications for acoustic wave RF filters according to an example of the present invention. The application chart 6100 for 5.2 GHz BAW RF filters shows mobile devices, smartphones, automobiles, Wi-Fi tri-band routers, tri-band mobile devices, tri-band smartphones, integrated cable modems, Wi-Fi tri-band access points, LTE/LAA small cells, and the like. A schematic representation of the frequency spectrum used in a tri-band Wi-Fi system is provided in FIG. 62.

FIG. 62 is a simplified diagram illustrating application areas for 5.2 GHz RF filters in Tri-Band Wi-Fi radios according to examples of the present invention. As shown, RF filters used by communication devices 6210 can be configured for specific applications at three separate bands of operation. In a specific example, application area 6220 operates at 2.4 GHz and includes computing and mobile devices, application area 6230 operates at 5.2 GHz and includes television and display devices, and application area 6240 operates at 5.6 GHz and includes video game console and handheld devices. Those of ordinary skill in the art will recognize other variations, modifications, and alternatives.

The present invention includes resonator and RF filter devices using both textured polycrystalline piezoelectric materials (deposited using PVD methods) and single crystal piezoelectric materials (grown using CVD technique upon a seed substrate). Various substrates can be used for fabricating the acoustic devices, such silicon substrates of various crystallographic orientations and the like. Additionally, the present method can use sapphire substrates, silicon carbide substrates, gallium nitride (GaN) bulk substrates, or aluminum nitride (AlN) bulk substrates. The present method can also use GaN templates, AlN templates, and AlxGa1-xN templates (where x varies between 0.0 and 1.0). These substrates and templates can have polar, non-polar, or semi-polar crystallographic orientations. Further the piezoelectric materials deposed on the substrate can include allows selected from at least one of the following: AlN, AlN, GaN, InN, InGaN, AlInN, AlInGaN, ScAlN, ScAlGaN, ScGaN, ScN, BAlN, BAlScN, and BN.

The resonator and filter devices may employ process technologies including but not limited to Solidly-Mounted Resonator (SMR), Film Bulk Acoustic Resonator (FBAR), or Single Crystal Bulk Acoustic Resonator (XBAW). Representative cross-sections are shown below in FIGS. 63A-63C. For clarification, the terms “top” and “bottom” used in the present specification are not generally terms in reference of a direction of gravity. Rather, the terms “top” and “bottom” are used in reference to each other in the context of the present device and related circuits. Those of ordinary skill in the art will recognize other variations, modifications, and alternatives.

In an example, the piezoelectric layer ranges between 0.1 and 2.0 um and is optimized to produced optimal combination of resistive and acoustic losses. The thickness of the top and bottom electrodes range between 250.ANG. and 2500.ANG. and the metal consists of a refractory metal with high acoustic velocity and low resistivity. The resonators are “passivated” with a dielectric (not shown in FIGS. 63A-63C) consisting of a nitride and or an oxide and whose range is between 100.ANG. and 2000.ANG. The dielectric layer is used to adjust resonator resonance frequency. Extra care is taken to reduce the metal resistivity between adjacent resonators on a metal layer called the interconnect metal. The thickness of the interconnect metal ranges between 500.ANG. and 5 um. The resonators contain at least one air cavity interface in the case of SMRs and two air cavity interfaces in the case of FBARs and XBAWs. The shape of the resonators selected come from assymetrical shapes including ellipses, rectanges, and polygons. Further, the resonators contain reflecting features near the resonator edge on one or both sides of the resonator.

FIGS. 63A-63C are simplified diagrams illustrating cross-sectional views of resonator devices according to various examples of the present invention. More particularly, device 6301 of FIG. 63A shows a BAW resonator device including an SMR, FIG. 63B shows a BAW resonator device including an FBAR, and FIG. 63C shows a BAW resonator device with a single crystal XBAW. As shown in SMR device 6301, a reflector device 6320 is configured overlying a substrate member 6310. The reflector device 6320 can be a Bragg reflector or the like. A bottom electrode 6330 is configured overlying the reflector device 6320. A polycrystalline piezoelectric layer 6340 is configured overlying the bottom electrode 6330. Further, a top electrode 6350 is configured overlying the polycrystalline layer 6340. As shown in the FBAR device 6302, the layered structure including the bottom electrode 6330, the polycrystalline layer 6340, and the top electrode 6350 remains the same. The substrate member 6311 includes an air cavity 6312, and a dielectric layer is formed overlying the substrate member 6311 and covering the air cavity 6312. As shown in XBAW device 6303, the substrate member 6311 also contains an air cavity 6312, but the bottom electrode 6330 is formed within a region of the air cavity 6312. A single crystal piezoelectric layer is formed overlying the substrate member 6311, the air cavity 6312, and the bottom electrode 6341. Further, a top electrode 6350 is formed overlying a portion of the single crystal layer 6341. These resonators can be scaled and configured into circuit configurations shown in FIGS. 64A-64C.

The RF filter circuit can comprise various circuit topologies, including modified lattice (“I”) 6401, lattice (“II”) 6402, and ladder (“III”) 6403 circuit configurations, as shown in FIGS. 64A, 64B, and 64C, respectively. These figures are representative lattice and ladder diagrams for acoustic filter designs including resonators and other passive components. The lattice and modified lattice configurations include differential input ports 6410 and differential output ports 6450, while the ladder configuration includes a single-ended input port 6411 and a single-ended output port 6450. In the lattice configurations, nodes are denoted by top nodes (t1-t3) and bottom nodes (b1-b3), while in the ladder configuration the nodes are denoted as one set of nodes (n1-n4). The series resonator elements (in cases I, II, and III) are shown with white center elements 6421-6424 and the shunt resonator elements have darkened center circuit elements 6431-6434. The series elements resonance frequency is higher than the shunt elements resonance frequency in order to form the filter skirt at the pass-band frequency. The inductors 6441-6443 shown in the modified lattice circuit diagram (FIG. 64A) and any other matching elements can be included either on-chip (in proximity to the resonator elements) or off-chip (nearby to the resonator chip) and can be used to adjust frequency pass-band and/or matching of impedance (to achieve the return loss specification) for the filter circuit. The filter circuit contains resonators with at least two resonance frequencies. The center of the pass-band frequency can be adjusted by a trimming step (using an ion milling technique or other like technique) and the shape the filter skirt can be adjusted by trimming individual resonator elements (to vary the resonance frequency of one or more elements) in the circuit.

In an example, the present invention provides an RF filter circuit device in a ladder configuration. The device can include an input port, a first node coupled to the input port, a first resonator coupled between the first node and the input port. A second node is coupled to the first node and a second resonator is coupled between the first node and the second node. A third node is coupled to the second node and a third resonator is coupled between the second node and the third node. A fourth node is coupled to the third node and a fourth resonator is coupled between the third node and the output port. Further, an output port is coupled to the fourth node. Those of ordinary skill in the art will recognize other variations, modifications, and alternatives.

Each of the first, second, third, and fourth resonators can include a capacitor device. Each such capacitor device can include a substrate member, which has a cavity region and an upper surface region contiguous with an opening in the first cavity region. Each capacitor device can include a bottom electrode within a portion of the cavity region and a piezoelectric material overlying the upper surface region and the bottom electrode. Also, each capacitor device can include a top electrode overlying the single crystal material and the bottom electrode, as well as an insulating material overlying the top electrode and configured with a thickness to tune the resonator.

The device also includes a serial configuration includes the input port, the first node, the first resonator, the second node, the second resonator, the third node, the third resonator, the fourth resonator, the fourth node, and the output port. A separate shunt configuration resonator is coupled to each of the first, second, third, fourth nodes. A parallel configuration includes the first, second, third, and fourth shunt configuration resonators. Further, a circuit response can be configured between the input port and the output port and configured from the serial configuration and the parallel configuration to achieve a transmission loss from a pass-band having a characteristic frequency centered around 5.2 GHz and having a bandwidth from 5.170 GHz to 5.330 GHz such that the characteristic frequency centered around 5.2 GHz is tuned from a lower frequency ranging from about 4 GHz to 5.1 GHz.

In a specific example, the first, second, third, and fourth piezoelectric materials are each essentially a single crystal aluminum nitride bearing material or aluminum scandium nitride bearing material, a single crystal gallium nitride bearing material or gallium aluminum bearing material, or the like. In another specific embodiment, these piezoelectric materials each comprise a polycrystalline aluminum nitride bearing material or aluminum scandium bearing material, or a polycrystalline gallium nitride bearing material or gallium aluminum bearing material, or the like.

In a specific example, the serial configuration forms a resonance profile and an anti-resonance profile. The parallel configuration also forms a resonance profile and an anti-resonance profile. These profiles are such that the resonance profile from the serial configuration is off-set with the anti-resonance profile of the parallel configuration to form the pass-band.

In a specific example, the pass-band is characterized by a band edge on each side of the pass-band and having an amplitude difference ranging from 10 dB to 60 dB. The pass-band has a pair of band edges; each of which has a transition region from the pass-band to a stop band such that the transition region is no greater than 250 MHz. In another example, pass-band can include a pair of band edges and each of these band edges can have a transition region from the pass-band to a stop band such that the transition region ranges from 5 MHz to 250 MHz.

In a specific example, each of the first, second, third, and fourth insulating materials comprises a silicon nitride bearing material or an oxide bearing material configured with a silicon nitride material an oxide bearing material.

In a specific example, the present device can further include several features. The device can further include a rejection band at a frequency greater than the pass-band. This rejection band can range from 5.490 GHz to 5.835 GHz. The device can further include an insertion loss of 2.1 dB and an amplitude variation characterizing the pass-band of 0.7 dB. Also, the device can include an attenuation of up to 40 dB for a frequency range of 1 GHz to 5 GHz or an attenuation of up to 48 dB for a frequency range of 5.9 GHz to 11 GHz. The device can further include a return loss characterizing the pass-band of up to 15 dB and the device can be operable from −40 Degrees Celsius to 85 Degrees Celsius. The device can further include a maximum power within the pass-band of 30 dBm or 1 Watt. Further, the pass-band can be configured for a U-NII-1+U-NII-2.ANG. bands and for an IEEE 802.11a channel plan.

In a specific example, the present device can be configured as a bulk acoustic wave (BAW) filter device. Each of the first, second, third, and fourth resonators can be a BAW resonator. Similarly, each of the first, second, third, and fourth shunt resonators can be BAW resonators. The present device can further include one or more additional resonator devices numbered from N to M, where N is four and M is twenty. Similarly, the present device can further include one or more additional shunt resonator devices numbered from N to M, where N is four and M is twenty.

In an example, the present invention provides an RF circuit device in a lattice configuration. The device can include a differential input port, a top serial configuration, a bottom serial configuration, a first lattice configuration, a second lattice configuration, and a differential output port. The top serial configuration can include a first top node, a second top node, and a third top node. A first top resonator can be coupled between the first top node and the second top node, while a second top resonator can be coupled between the second top node and the third top node. Similarly, the bottom serial configuration can include a first bottom node, a second bottom node, and a third bottom node. A first bottom resonator can be coupled between the first bottom node and the second bottom node, while a second bottom resonator can be coupled between the second bottom node and the third bottom node.

In an example, the first lattice configuration includes a first shunt resonator cross-coupled with a second shunt resonator and coupled between the first top resonator of the top serial configuration and the first bottom resonator of the bottom serial configuration. Similarly, the second lattice configuration can include a first shunt resonator cross-coupled with a second shunt resonator and coupled between the second top resonator of the top serial configuration and the second bottom resonator of the bottom serial configuration. The top serial configuration and the bottom serial configuration can each be coupled to both the differential input port and the differential output port.

In a specific example, the device further includes a first balun coupled to the differential input port and a second balun coupled to the differential output port. The device can further include an inductor device coupled between the differential input and output ports. In a specific example, the device can further include a first inductor device coupled between the first top node of the top serial configuration and the first bottom node of the bottom serial configuration; a second inductor device coupled between the second top node of the top serial configuration and the second bottom node of the bottom serial configuration; and a third inductor device coupled between the third top node of the top serial configuration and the third bottom node of the bottom serial configuration.

The packaging approach includes but is not limited to wafer level packaging (WLP), WLP-plus-cap wafer approach, flip-chip, chip and bond wire, as shown in FIGS. 65 and 66. One or more RF filter chips and one or more filter bands can be packaged within the same housing configuration. Each RF filter band within the package can include one or more resonator filter chips and passive elements (capacitors, inductors) can be used to tailor the bandwidth and frequency spectrum characteristic. For a tri-band Wi-Fi system application, a package configuration including three RF filter bands, including the 2.4 GHz, 5.2 GHz, and 5.6 GHz band-pass solutions is capable using the BAW RF filter technology. The 2.4 GHz filter solution can be either surface acoustic wave (SAW) or BAW, whereas the 5.2 GHz and 5.6 GHz bands are likely BAW given the high-frequency capability of BAW.

FIG. 65A is a simplified diagram illustrating a packing approach according to an example of the present invention. As shown, device 6501 is packaged using a conventional die bond of an RF filter die 6510 to the base 6520 of a package and metal bond wires 6530 to the RF filter chip from the circuit interface 6540.

FIG. 65B is as simplified diagram illustrating a packing approach according to an example of the present invention. As shown, device 6602 is packaged using a flip-mount wafer level package (WLP) showing the RF filter silicon die 6510 mounted to the circuit interface 6540 using copper pillars 6531 or other high-conductivity interconnects.

FIG. 66 is a simplified diagram illustrating a packing approach according to an example of the present invention. Device 6600 shows an alternate version of a WLP utilizing a BAW RF filter circuit MEMS device 6630 and a substrate 6610 to a cap wafer 6640. In an example, the cap wafer 6640 may include thru-silicon-vias (TSVs) to electrically connect the RF filter MEMS device 6630 to the topside of the cap wafer (not shown in the figure). The cap wafer 6640 can be coupled to a dielectric layer 6620 overlying the substrate 6610 and sealed by sealing material 6650.

In an example, the present filter passes frequencies in the range of 5.17 to 5.33 GHz and rejects frequencies outside of this pass-band. Additional features of the 5.2 GHz acoustic wave filter circuit are provided below. The circuit symbol which is used to reference the RF filter building block is provided in FIG. 67. The electrical performance specifications of the 5.2 GHz filter are provided in FIG. 68 and the pass-band performance of the filter is provided in FIG. 69.

In various examples, the present filter can have certain features. The die configuration can be less than 2 mm.times.2 mm.times.0.5 mm; in a specific example, the die configuration is typically less than 1 mm.times. 1 mm.times.0.2 mm. The packaged device has an ultra-small form factor, such as a 2 mm.times.2.5 mm.times.0.9 mm using a conventional chip and bond wire approach, shown in FIG. 65. WLP package approaches can provide smaller form factors. In a specific example, the device is configured with a single-ended 50-Ohm antenna, and transmitter/receiver (Tx/Rx) ports. The high rejection of the device enables coexistence with adjacent Wi-Fi UNIT bands. The device is also be characterized by a high power rating (maximum+30 dBm), a low insertion loss pass-band filter with less than 2.5 dB transmission loss, and performance over a temperature range from −40 degrees Celsius to +85 degrees Celsius. Further, in a specific example, the device is RoHS (Restriction of Hazardous Substances) compliant and uses Pb-free (lead-free) packaging.

FIG. 67 is a simplified circuit diagram illustrating a 2-port BAW RF filter circuit according to an example of the present invention. As shown, circuit 6700 includes a first port (“Port 1”) 6711, a second port (“Port 2”) 6712, and a filter 6720. The first port represents a connection from a transmitter (TX) or received (RX) to the filter 6720 and the second port represents a filter connection from the filter 6720 to an antenna (ANT).

FIG. 68 is a simplified table of filter parameters according to an example of the present invention. As shown, table 6800 includes electrical specifications for a 5.2 GHz RF resonator filter circuit. The circuit parameters are provided along with the specification units, minimum, along with typical and maximum specification values.

FIG. 69 is a simplified graph representing insertion loss over frequency according to an example of the present invention. As shown, graph 6900 represents a narrowband measured vs. modeled response for 5.2 GHz RF filter using a ladder RF filter circuit configuration. The modeled curve 6910 is the transmission loss (s21) predicted from a linear simulation tool incorporation non-linear, full 3-dimensional (3D) electromagnetic (EM) simulation. The measured curve 6920 is the s21 measured from scattering parameters (s-parameters) taken from a network analyzer test system.

In an example, the present invention provides a front end module (FEM) for a 5.2 GHz Wi-Fi acoustic wave resonator RF filter circuit. The device can include a power amplifier (PA), a 5.2 GHz resonator, and a diversity switch. In a specific example, the device can further include a low noise amplifier (LNA). The PA is electrically coupled to an input node and can be configured to a DC power detector or an RF power detector. The resonator can be configured between the PA and the diversity switch, or between the diversity switch and an antenna. The LNA may be configured to the diversity switch or be electrically isolated from the switch. Another 5.2 GHZ resonator may be configured between the diversity switch and the LNA. In a specific example, this device integrates a 5.2 GHz PA, a 5.2 GHZ bulk acoustic wave (BAW) RF filter, a single pole two throw (SP2T) switch, and an optional bypassable low noise amplifier (LNA) into a single device. FIGS. 70-74 show five examples of FEMS according to various embodiments of the present invention. In each example, the LNA may be omitted to produce a transmit module only. In the following figures, the reference number scheme for the elements of these FEMs remains the same across FIGS. 70-74 except for the first two digits that correspond to the figure number.

FIG. 70 is a simplified circuit block diagram illustrating a front end module according to an example of the present invention. As shown, device 7000 includes a PA 7010, a 5.2 GHz resonator 7020, a diversity switch 7030, and an LNA 7040. Here, the input of the PA 7010 is electrically coupled to an input node (shown as TX_IN [2]). In a specific example, the PA can be a 5.2 GHz PA. An inductor 7011 can electrically coupled to the input node as well. The 5.2 GHz resonator 7020 is electrically coupled to the output of the PA 7010. In specific example, the resonator 7020 can be a 5.2 BAW resonator.

The diversity switch 7030 shown here is a single pole two throw (SP2T) switch. One of the throws is electrically coupled to the 5.2 GHz resonator 7020 while the other throw is electrically coupled to an output node (shown as RX OUT [14]). In a specific example, a coupling capacitor 7031 can be configured between the switch 7030 and the output node. The pole, which can switch between the two throws, is electrically coupled to an antenna (shown as ANT [12]). In a specific example, a coupling capacitor 7032 can be configured between the switch 7030 and the antenna.

In this case, the LNA 7040 is configured separately from the previous circuit elements and is electrically coupled to an LNA input (shown as LNA_IN [16]) and an LNA output (shown as LNA_OUT [17]). As previously discussed, the LNA 7040 may be omitted, which would result in a device that is a transmit module only. In a specific embodiment, coupling capacitors 7041 and 7042 can be configured between the LNA 7040 and the LNA input and LNA output, respectively. A signal filter 7043 can be configured between the LNA and coupling capacity 7041. In this case, the signal filter 7043 is a bandstop filter. Further, the LNA 7040 can be configured in a switched feedback loop 7044. In a specific example, the LNA 7040 can be a bypassable LNA.

In an example, the device 7000 can be configured with a power detector, which can be a DC power detector or an RF power detector. A DC power detector has a voltage output and would be electrically coupled to the PA at a DC power detect node (shown as DC_PDET [6]). In a specific example, a diode is configured between the PA and the DC power detector. An RF power detector has an RF output from a directional coupler 7013, which is configured at the output of the PA.

In an example, the present device design provides a compact form factor and integrated matching minimizes layout area in applications. The PA can be optimized for a 5V supply voltage that conserves power consumption while maintaining a high linear output power and throughput. Also, an integrated BAW filter reduces the overall size for Wi-Fi radio applications and allows coexistence between the 5.2 GHz radio band and adjacent 2.4 GHz and 5.6 GHz bands in a tri-band router configuration. Those of ordinary skill in the art will recognize other variations, modifications, and alternatives to the above.

FIG. 71 is a simplified circuit block diagram illustrating a front end module according to an example of the present invention. The reference number scheme is the same as in FIG. 70 except that the first two digits referencing “71.” As shown, device 7100 is similar to device 7000 of FIG. 70 except for the configuration of the 5.2 GHz resonator 7120. Here, the resonator 7120 is configured between the pole of the diversity switch 7130 and the antenna, as well as the coupling capacitor 7132. Of course, there can be other variations, modifications, and alternatives.

FIG. 72 is a simplified circuit block diagram illustrating a front end module according to an example of the present invention. The reference number scheme is the same as in FIG. 70 except that the first two digits reference “72.” As shown, device 7200 is similar to device 7000 except that there is an additional 5.2 GHz resonator 7221 configured between one of the throws of the diversity switch 7230 and the input to the LNA 7240, as well as the signal filter 7243. In this example, the switch 7230 is not coupled to the output node, and the LNA is not coupled to the LNA input node. Similar to the first resonator 7220, the second resonator 7221 can also be a 5.2 GHz BAW resonator. Of course, there can be other variations, modifications, and alternatives.

FIG. 73 is a simplified circuit block diagram illustrating a front end module according to an example of the present invention. The reference number scheme is the same as in FIG. 70 except that the first two digits reference “73.” As shown, device 7300 is similar to device 7200 of FIG. 72 except that the diversity switch 7330 is a single pole three throw (SP3T) switch and the LNA 7340 no longer includes the switched feedback loop. Rather, the output of the LNA 7340 is electrically coupled to the third throw of the switch 7340. Of course, there can be other variations, modifications, and alternatives.

FIG. 74 is a simplified circuit block diagram illustrating a front end module according to an example of the present invention. The reference number scheme is the same as in FIG. 70 except that the first two digits reference “74.” As shown, device 7400 is similar to device 7100 of FIG. 71 by having the 5.2 GHz resonator 7420 configured between the switch 7030 and the antenna, but also similar to device 7300 of FIG. 73 by having the output of the LNA 7440 electrically coupled to a third throw of switch 7430, which is a SP3T switch. Of course, there can be other variations, modifications, and alternatives.

As appreciated by the present inventors, in some embodiments according to the invention, piezoelectric based BAW resonator filters described above (for example, in reference to FIG. 64A-C) may be further improved by replacing the resonator 6421 with (or the addition of) a rejection-band series resonator that is configured to have an anti-resonant frequency in a rejection-band of frequencies that is below the pass-band. In some approaches a rejection-band shunt resonator can be added across the input to the resonator 6421, where the rejection-band shunt resonator is configured to have a resonant frequency in a rejection-band that is above the pass-band. It will be understood that the anti-resonant frequencies of the rejection-band series resonators coupled to the inputs and the outputs of the filter can be different and may overlap one another. Still further, the resonant frequencies of the rejection-band shunt resonators coupled to the inputs and the outputs of the filter can be different and may overlap one another.

Accordingly, BAW resonator filters according to embodiments of the invention can be utilized to improve the rejection band performance of filters configured to provide a pass-band of 5.17 GHz to 5.33 GHz. BAW resonator filters according to embodiments of the invention can also be utilized to improve the rejection band performance of filters configured to provide a pass-band of 5.49 GHz to 5.835 GHz. It will be understood that embodiments according to the invention may be provided by the inclusion of at least one rejection-band series or shunt resonator coupled to either the input or the output of a BAW resonator filter. Further, a BAW resonator filter can be any topology filter circuit, such as a ladder or lattice topology.

In still other embodiments, a BAW resonator filter that includes the rejection-band series resonators can be combined with a BAW resonator filter that includes the rejection-band shunt resonators along with a switch to select one of the BAW resonator filters for operation. For example, in a first state the switch may couple an input signal to the BAW resonator filter that includes the rejection-band series resonators, whereas in a second state the switch may couple the input signal to the BAW resonator filter that includes the rejection-band shunt resonators. Accordingly, in some embodiments two different BAW resonator filters (each having a different pass-band of frequencies) can be integrated into a single device where the switch can be used to select the particular BAW resonator filter for a particular application.

It will be further understood that the rejection-band series resonators can be formed using a rejection-band mass load structure that is greater in mass than a pass-band mass load structure on the pass-band series resonators. Accordingly, methods used to form the pass-band resonators can be adapted to form the rejection-band series resonators described herein by increasing the mass loading on the rejection band resonator relative to that used to form the pass-band resonators. For example, the first rejection-band series resonators can be formed with a rejection-band mass load structure that is greater in mass than a pass-band mass load structure on the pass-band shunt resonators. Still further, the rejection-band series resonator can include a rejection-band mass load structure that is greater in mass than the pass-band mass load structure.

FIG. 75 is a schematic illustration of a BAW resonator filter 7500 including a BAW resonator pass-band filter ladder 7505 and first and second rejection-band series resonators 7510 and 7515 in some embodiments according to the invention. According to the FIG. 75, an input node of the BAW resonator pass-band filter ladder 7505 is coupled to the first rejection-band series resonator 7510 and an output node of the BAW resonator pass-band filter ladder 7505 is coupled to the second rejection-band series resonator 7515.

FIG. 76 is a graph illustrating anti-resonant frequencies of first and second rejection-band series resonators 7510 and 7515 in the BAW resonator filter of FIG. 75 in some embodiments according to the invention. According to FIG. 76, the BAW resonator filter of FIG. 75 provides a pass-band filter with a pass-band frequency range of about 5.49 GHz to about 5.835 GHz. The first and second rejection-band series resonators 7510 and 7515 are configured to provide anti-resonant frequency peaks 7520 and 7525 and rejection nulls 7607 and 7608 below and adjacent to the lower edge of the pass-band. It will be understood that although the rejection nulls 7607 and 7608 in FIG. 76 are below and adjacent to the lower edge of the pass-band, in some embodiments the corresponding rejection nulls may be below but not necessarily adjacent to the lower edge of the pass-band. In some embodiments, the anti-resonant frequencies peaks 7520 and 7525 are approximately aligned with the rejection nulls 7607 and 7608 in the BAW resonator filter response 7524 in the rejection-band of frequencies that are below and adjacent to a lower edge of the pass-band of frequencies.

As described herein, in some embodiments according to the invention the resonant or anti-resonant frequency peaks associated with series or shunt rejection band resonators can be aligned with rejection nulls exhibited in the response of the filter circuit. It will be understood, however, that in some embodiments the resonant or anti-resonant frequency peaks associated with series or shunt rejection band resonators can provide the rejection nulls as part of the filter response without alignment to otherwise existing rejection nulls included in the filter response.

As appreciated by the present inventors, the alignment of the anti-resonant frequencies peaks 7520 and 7525 from first and second rejection-band series resonators 7510 and 7515 with the rejection nulls in the filter response can provide a combined attenuation in the rejection-band of frequencies that is greater than the attenuation that would be provided without the inclusion of the first and second rejection-band series resonators 7510 and 7515, as illustrated by the filter response 7524 in FIG. 76. In some embodiments, the inclusion of the rejection-band series resonators 7510 and 7515, with the alignment described herein, can provide at least about an additional 5 dB of the attenuation that would be provided without the inclusion of the first and second rejection-band series resonators 7510 and 7515. In some embodiments, the inclusion of the rejection-band series resonators 7510 and 7515, with the alignment described herein, can provide at least about an additional 10 dB of attenuation to the filter response.

In some embodiments the resonant frequency peaks 7526 of the pass-band series resonators and the anti-resonant frequency peaks 7530 of the pass-band shunt resonators are located at about a center of the pass-band of frequencies. Still further, the resonant frequency peaks 7535 of the pass-band shunt resonators are located below or at about the lower edge of the pass-band and the anti-resonant frequency peaks 7609 and 7610 of the pass-band series resonators are located at about or above an upper edge of the pass-band.

FIG. 80 is a schematic illustration of a BAW resonator filter including the BAW resonator pass-band filter lattice of FIG. 64A including first and second rejection-band series resonators 8010 and 8015 in some embodiments according to the invention. FIG. 81 is a schematic illustration of a BAW resonator filter including the BAW resonator pass-band filter lattice of FIG. 64B including first and second rejection-band series resonators 8110 and 8115 in some embodiments according to the invention. According to FIGS. 80 and 81, the first and second rejection-band series resonators can also be added to the input and output nodes, respectively, of a BAW resonator pass-band filter lattice, such as that shown in FIGS. 64A and 64B, to further improve the rejection performance.

FIG. 82 is a graph representative of the BAW resonator filter response 8420 of FIGS. 80 and 81 including the anti-resonant frequencies of the first and second rejection-band series resonators 8010/8015 and 8110/8115 in some embodiments according to the invention. According to FIG. 82 the anti-resonance frequency peaks 8225 and 8220 associated with the first and second rejection-band series resonators 8010/8015 and 8110/8115 can be approximately aligned with the rejection nulls 7607 and 7608 in the BAW resonator filter response 8240 in the rejection-band of frequencies that are below and adjacent to a lower edge of the pass-band of frequencies. It will be understood that although the rejection nulls 7607 and 7608 in FIG. 82 are below and adjacent to the lower edge of the pass-band, in some embodiments the corresponding rejection nulls may be below but not necessarily adjacent to the lower edge of the pass-band. As appreciated by the present inventors, the alignment of the anti-resonant frequency peaks from first and second rejection-band series resonators 8010/8015 and 8110/8115 with the rejection nulls 7607 and 7608 can provide a combined attenuation in the rejection-band of frequencies that is greater than the attenuation that would be provided without the inclusion of the first and second rejection-band series resonators 8010/8015 and 8110/8115. In some embodiments, the inclusion of the rejection-band series resonators 8010/8015 and 8110/8115, with the alignment described herein, can provide at least about an additional 5 dB of the attenuation that would be provided without the inclusion of the first and second rejection-band series resonators 8010/8015 and 8110/8115. In some embodiments, the inclusion of the rejection-band series resonators 8010/8015 and 8110/8115, with the alignment described herein, can provide at least about an additional 10 dB of attenuation.

FIG. 77 is a schematic illustration of a BAW resonator filter 7700 including a BAW resonator pass-band filter ladder 7705 and first and second rejection-band shunt resonators 7710 and 7715 in some embodiments according to the invention. According to the FIG. 77, an input node of the BAW resonator pass-band filter ladder 7505 is coupled to the first rejection-band shunt resonator 7710 and an output node of the BAW resonator pass-band filter ladder 7505 is coupled to the second rejection-band shunt resonator 7515.

FIG. 78 is a graph illustrating resonant frequencies of first and second rejection-band shunt resonators 7710 and 7715 in the BAW resonator filter 7700 of FIG. 77 in some embodiments according to the invention. According to FIG. 78, the BAW resonator filter of FIG. 77 provides a pass-band filter with a pass-band frequency range of about 5.17 GHz to about 5.33 GHz. The first and second rejection-band shunt resonators 7710 and 7715 are configured to provide resonant frequency peaks 7805 and 7806 and can be aligned with rejection nulls 7807 and 7808 in the filter response 7824 above the pass-band. It will be understood that although the rejection nulls 7807 and 7808 in FIG. 78 are above the pass-band, in some embodiments the corresponding rejection nulls may be adjacent to and above the upper edge of the pass-band. In some embodiments the resonant frequency peaks 7815 of the pass-band series resonators and the anti-resonant frequency peaks 7810 of the pass-band shunt resonators are located at about a center of the pass-band of frequencies. Still further, the resonant frequency peaks 7820 of the pass-band shunt resonators are located below a lower edge of the pass-band and the anti-resonant frequency peaks 7811 and 7812 of the pass-band series resonators can be located above and adjacent to an upper edge of the pass-band.

As appreciated by the present inventors, the alignment of the resonant frequencies peaks 7805 and 7806 from first and second rejection-band shunt resonators 7710 and 7715 with the rejection nulls 7807 and 7808 in the filter response can provide a combined attenuation in the rejection-band of frequencies that is greater than the attenuation that would be provided without the inclusion of the first and second rejection-band shunt resonators 7710 and 7715. In some embodiments, the inclusion of the rejection-band shunt resonators 7710 and 7715, with the alignment described herein, can provide at least about an additional 5 dB of the attenuation that would be provided without the inclusion of the first and second rejection-band shunt resonators 7710 and 7715. In some embodiments, the inclusion of the rejection-band shunt resonators 7710 and 7715, with the alignment described herein, can provide at least about an additional 10 dB of attenuation.

FIG. 83 is a schematic illustration of a BAW resonator filter including the BAW resonator pass-band filter lattice 6401 of FIG. 64A including first and second rejection-band shunt resonators 8310 and 8315 in some embodiments according to the invention. FIG. 84 is a schematic illustration of a BAW resonator filter including the BAW resonator pass-band filter lattice 6402 of FIG. 64B including first and second rejection-band shunt resonators 8410 and 8415 in some embodiments according to the invention. According to FIGS. 83 and 84, the first and second rejection-band shunt resonators can also be added to the input and output nodes, respectively, of a BAW resonator pass-band filter lattice, such as that shown in FIGS. 64A and 64B, to further improve the rejection performance.

FIG. 85 is a graph representative of the BAW resonator filter response 8524 of FIGS. 83 and 84 including the resonant frequencies of the first and second rejection-band shunt resonators 8310/8315 and 8410/8415 in some embodiments according to the invention. According to FIG. 85 the resonant frequency peaks 7805 and 7806 associated with the first and second rejection-band shunt resonators 8310/8315 and 8410/8415 can be approximately aligned with the rejection nulls 7807 and 7808 in the BAW resonator filter response 8524 in the rejection-band of frequencies that are above an upper edge of the pass-band of frequencies. It will be understood that although the rejection nulls 7807 and 7808 in FIG. 85 are above the pass-band, in some embodiments the corresponding rejection nulls may be adjacent to and above the upper edge of the pass-band. As appreciated by the present inventors, the alignment of the resonant frequency peaks from first and second rejection-band shunt resonators 8310/8315 and 8410/8415 with the rejection nulls 8707 band 8708 can provide a combined attenuation in the rejection-band of frequencies that is greater than the attenuation that would be provided without the inclusion of the first and second rejection-band shunt resonators 8310/8315 and 8410/8415. In some embodiments, the inclusion of the rejection-band shunt resonators 8310/8315 and 8410/8415, with the alignment described herein, can provide at least about an additional 5 dB of the attenuation that would be provided without the inclusion of the first and second rejection-band shunt resonators 8310/8315 and 8410/8415. In some embodiments, the inclusion of the rejection-band shunt resonators 8310/8315 and 8410/8415, with the alignment described herein, can provide at least about an additional 10 dB of attenuation.

FIG. 79 is a schematic illustration of a combined BAW resonator filter 7900 including a BAW resonator pass-band filter ladder 7505 coupled to first and second rejection-band series resonators and a BAW resonator pass-band filter ladder 7705 coupled to first and second rejection-band shunt resonators. The input and output of BAW resonator pass-band filter ladder 7505 and the BAW resonator pass-band filter ladder 7705 are controlled by setting the switches 7905/7910 in some embodiments according to the invention. According to FIG. 79, in a first state the switches 7905/7910 may couple the input signal to the BAW resonator pass-band filter ladder 7505 via the input rejection-band series resonator and couple the output of the BAW resonator pass-band filter ladder 7505 to the output signal of the BAW resonator filter 7900 via the output rejection-band series resonator, whereas in a second state the switches 7905/7910 may couple the input signal to the BAW resonator pass-band filter ladder 7705 via the input rejection-band shunt resonator and couple the output of the BAW resonator pass-band filter ladder 7705 to the output signal of the BAW resonator filter 7900 via the output rejection-band shunt resonator. Although the combined BAW resonator filter 7900 of FIG. 79 shows first and second ladder type filter circuit topology, it will be understood that any topology filter circuit, such as a lattice or modified lattice, may also be used in some embodiments according to the invention. Still further, in some embodiments, a combination of ladder filter circuits and lattice filter circuits may be included in the BAW resonator filter 7900. Still further, more than two filter circuits may be included in the BAW resonator filter 7900 along with more switches that are configured and operated to select the filter to be used.

While the above is a full description of the specific embodiments, various modifications, alternative constructions and equivalents may be used. As an example, the packaged device can include any combination of elements described above, as well as outside of the present specification. Therefore, the above description and illustrations should not be taken as limiting the scope of the present invention which is defined by the appended claims. 

What is claimed:
 1. A Bulk Acoustic Wave (BAW) resonator filter comprising: a BAW resonator pass-band filter circuit, the BAW resonator pass-band filter circuit configured to pass frequency components of an input signal in a pass-band of frequencies received at an input node of the BAW resonator pass-band filter circuit to an output node of the BAW resonator pass-band filter circuit; a first rejection-band series resonator coupled in series between an input port of the BAW resonator pass-band filter circuit and the input node, the first rejection-band series resonator having a first anti-resonant frequency peak in a rejection-band of frequencies that is less than the pass-band of frequencies; and a second rejection-band series resonator coupled in series between an output port of the BAW resonator filter and the output node, the second rejection-band series resonator having a second anti-resonant frequency peak in the rejection-band of frequencies.
 2. The BAW resonator filter of claim 1 wherein the BAW resonator pass-band filter circuit comprises a ladder topology, a lattice topology, or a modified lattice topology.
 3. The BAW resonator filter of claim 2 wherein the BAW resonator pass-band filter circuit comprises BAW resonator pass-band filter ladder including: a plurality of pass-band series resonators coupled in series between the, input node and the output node, the pass-band series resonators having respective resonant frequency peaks in the pass-band of frequencies; and a plurality of pass-band shunt resonators coupled in parallel with the input node and a reference node or in parallel with the output node and the reference node of the BAW resonator filter, the pass-band shunt resonators having respective anti-resonant frequency peaks in the pass-band of frequencies.
 4. The BAW resonator filter of claim 3 wherein the respective resonant frequency peaks of the pass-band series resonators and the respective anti-resonant frequency peaks of the pass-band shunt resonators are at about a center of the pass-band of frequencies.
 5. The BAW resonator filter of claim 4 wherein the respective resonant frequency peaks of the pass-band shunt resonators are at about or less than a lower edge of the pass-band of frequencies and respective anti-resonant frequency peaks of the pass-band series resonators are at about or greater than an upper edge, of the pass-band of frequencies.
 6. The BAW resonator filter of claim 1 wherein the BAW resonator pass-band filter circuit provides first and second rejection nulls in the rejection-band of frequencies adjacent to a lower edge of the pass-band, of frequencies; and wherein the first and second an frequency peaks of tube first and second rejection-band series resonators are approximately aligned with the first and second rejection nulls at respective frequencies to provide a combined attenuation of the input signal in the rejection-band of frequencies at the respective frequencies.
 7. The BAW resonator filter of claim 6 wherein the first and second anti-resonant frequency peaks provide at least about an additional 5 dB attenuation of the combined attenuation.
 8. The BAW resonator filter of claim 1 wherein the first rejection-band series resonator includes a first rejection-hand mass load structure that is greater in mass than a pass band mass load structure on a pass-band shunt resonator included in the BAW resonator pass-band filter circuit.
 9. The BAW resonator filter of claim 8 wherein the second rejection-band series resonator includes a second rejection-band mass load structure that is greater in mass than the pass-band mass load structure on the pass-band shunt resonator included in the BAW resonator pass-band filter circuit.
 10. A Bulk Acoustic Wave (BAW) resonator filter comprising: a BAW resonator pass-band filter circuit, the BAW resonator pass-band filter circuit configured to pass frequency components of an input signal in a pass-band of frequencies received at an input port of the BAW resonator pass-band filter circuit to an output port of the BAW resonator pass-band filter circuit; a first rejection-band shunt resonator coupled in parallel across an input port of the BAW resonator pass-band filter circuit and a reference node of the BAW resonator pass-band filter circuit, the first rejection-band shunt resonator having a first resonant frequency peak in a rejection-band, of frequencies that is greater than the pass-band of frequencies; and a second rejection-band shunt resonator coupled in parallel between the output port of the BAW resonator filter and the reference node, the second rejection-band :shunt resonator having a second resonant frequency peak in the rejection-band of frequencies.
 11. The BAW resonator filter of claim 10 wherein the BAW resonator pass-band filter circuit comprises a ladder topology, a lattice topology, or a modified lattice topology.
 12. The BAW resonator filter of claim 11 wherein the BAW resonator pass-band filter circuit comprises BAW resonator pass-band filter ladder including: a plurality of pass-band series resonators coupled in series between the input port and the output port, the pass-band series resonators having respective resonant frequency peaks in the pass-band of frequencies; and a plurality of pass-band shunt resonators coupled in parallel with the input port and the reference node or in parallel with the output port and the reference node of the BAW resonator filter, the pass-band shunt resonators having respective anti-resonant frequency peaks in the pass-band of frequencies.
 13. The BAW resonator filter of claim 12 wherein the respective resonant frequency peaks of the pass-band series resonators and the respective anti-resonant frequency peaks of the pass-band shunt resonators are at about a center of the, pass-band of frequencies.
 14. The BAW resonator filter of claim 10 wherein the BAW resonator pass-band filter circuit provides first and second rejection nulls in the rejection-band of frequencies adjacent to an upper edge of the pass-band of frequencies; and wherein the first and second resonant frequency peaks of the first and second rejection-band shunt resonators are approximately aligned with the first and second rejection nulls at respective frequencies to provide a combined attenuation of the input signal in the rejection-band of frequencies at the respective frequencies.
 15. The BAW resonator filter of claim 14 wherein the first and second resonant frequency peaks provide at least about an additional 5 dB attenuation of the combined attenuation.
 16. The BAW resonator filter of claim 10 wherein the first rejection-band shunt resonator includes a first rejection-band mass load structure that is lesser in mass than a pass-band mass load structure on a pass-band series resonator included in the BAW resonator pass-band filter circuit.
 17. The BAW resonator filter of claim 16 wherein the second rejection-band shunt resonator includes a second rejection-band mass load structure that is lesser in mass than the pass-band mass load structure on the pass-band series resonator included in the BAW resonator pass-band filter circuit.
 18. The BAW resonator filter of claim 10 wherein the BAW resonator pass-band filter circuit comprises a BAW resonator pass-band filter ladder and the first rejection-band shunt resonator is coupled in parallel across the input port of the BAW resonator pass-band filter circuit and the reference node, the BAW resonator filter further comprising: a second rejection-band shunt resonator coupled in parallel between the output port of the BAW resonator pass-band filter circuit and the reference node, the second rejection-band shunt resonator having a second resonant frequency peak in the rejection-band of frequencies.
 19. A Bulk Acoustic Wave (BAW) resonator filter comprising: a first BAW resonator pass-band filter circuit configured to pass frequency components of an input signal of the BAW resonator filter in a first pass-band of frequencies received at an input port of the first BAW resonator pass-band filter circuit to an output port of the first BAW resonator pass-band filter circuit; a first rejection-band series resonator coupled in series with the input port of the first BAW resonator pass-band filter circuit or the output port of the first BAW resonator pass-band filter circuit, the first rejection-band series resonator having ,a first anti-resonant frequency peak in a first rejection-band of frequencies that is less than the first pass-band of frequencies; a second BAW resonator pass-band filter circuit configured to pass frequency components of the input signal in a second pass-band of frequencies received at an input port of the second BAW resonator pass-band filter circuit to an output port of the second BAW resonator pass-band filter circuit; a first rejection-band shunt resonator coupled in parallel across the input port of the second BAW resonator pass-band filter circuit and a reference node of the second BAW resonator pass-band filter circuit or coupled in parallel across the output port of the second BAW resonator pass-band filter circuit and the reference node of the second BAW resonator pass-band filter circuit, the first rejection-band shunt resonator having a first resonant frequency peak in a second rejection-band of frequencies that is greater than the second pass-band of frequencies; and a switch configured to couple the input signal to the input port of the first BAW resonator pass-band filter circuit and to couple the output port of the first BAW resonator pass-band filter circuit to an output signal of the BAW resonator filter in a first state, and configured to couple the input, signal to the input port of the second BAW resonator pass-band filter circuit and to couple the output port of the second BAW resonator pass-band filter circuit to the output signal of the BAW resonator filter in a second state.
 20. The BAW resonator filter of claim 19 wherein in the first state the first pass-band of frequencies is about 5.49 GHz to about 5.835 GHz and wherein the first rejection-band of frequencies is about 5.17 GHz to about 5.33 GHz. 